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Y.I.Perelman MIR PUBLISHERS MOSCOW In 1913 in Russian bookshops appeared a book by the outstanding educationalist Yakov Isidorovich Perelman entitled Physics for Entertainment. It ctruck the fancy of the young who found in it the r nswers to many of the question* that interested them. Physics for Entertainment not only had an interesting layout, it was also immensely instructive. In the preface to the 11th edition Perelman wrote: “The main objective of Physics for Entertainment is to arouse the activity of scientific imagination, to teach the reader to think in the spirit of the science of physics and to create in his mind a wide variety of associations of physical knowledge with the widely differing facts of life, with all that he normally comes in contact with* Physics for Entertainment was a best seller. Y. L Perelman was bom in 1882 in the town of Byelostok (now in Poland). In 1909 he obtained a diploma of forester from the St Petersburg Forestry Institute. After the success of Physics far Entertainment Perelman set out to produce other books, in which he showed himself to be an imajg^ative pppularizer of science. Especially popular were Arithmetics for Entertainment, Mechanics for Entertainment, Geometry for Entertainment, Astronomy for Entertainment lively Mathematics, Physics Everywhere, and Tricks and Amusements. Today tbe$e books are known to every educated person in the Soviet Union. He has also written several books on interplanetarytravel (Interplanetary Journeys, On a Rocket to Stars, World Expanses, etCjL • The great scientist ICE. TsioUcovsky thought hi^Uy of the talent and creative genius of Perelman. He wrote of him in the preface to Interplanetary Journeys: “The author has long been known by his popular, witty and quite scientific works on physics, astronomy and mathematics, which are moreover written in a marvelous language and are wry readable* Perelman has also authored a number of textbooks and articles in Soviet popular science magazines. In addition to his educational, scientific and literary activities, he has also devoted much time to editing. So he was the editor of the magazines Nature and People and In the Workshop of Nature. Perelman died on March 16, 1942, in Leningrad. Many generations of readers have enjoyed Perelman’s fascinating books, and they will undoubtedly be of interest for generations to come. Fun with Maths and Physics Brain Teasers Tricks Illusions MIR PUBLISHERS MOSCOW $1. H. IlepejibMaH 3AHHMATEJIbHbIE 3A/JAMH H OnbITbl M3,aaTejibCTBo «,Z^eTCKaji JiHTepaTypa», MocKBa Compiled by 1.1. Prusakov Translated from the Russian by Alexander Repyev Ha aneauuckom H3biKe © English translation, Mir Publishers, 1984 Cover: I. Kravtsov, V. Stulikov Artistic Book Design: 1. Kabakov, V. Keidan, 1. Kravtsov, D. Lion, S. Mukhin, Yu. Perevezentsev, L. Saksonov, A. Sokolov, V. Stulikov, R. Varshamov, Yu. Vashchenko c CONTENTS By the Way 33 gwAr For Young Physicists A Sheet of Newspaper 86 8-9 ® Seventy-Five More Questions Jlv? and Experiments m#* on Physics 100 Optical Illusions 143 Brain-Twisting Arrangements and Permutations 12-13 Problems with Squares Problems on Manual Work 188 Problems on Transport 211 18-19 Surprising Calculations 215 ¥ n f Problems from Gulliver's Travels 229 Stories about Giant Numbers 237 22-23 Tricks with Numbers 250 Merry Arithmetic 273 Fast Reckoning 289 t J 4\ 26\ 1 28 3o\ 6 52 7 r 36\ 26-27 Magic Squares 296 Arithmetic Games and Tricks 303 28-29 With a Stroke of the Pen 332 Geometric Recreations 338 r «3 30-31 Without a Tape-Measure m Simple. Tricks and Diversions 358 ^ Drawing Puzzles *7 6 32-33 By die Way Figure l Scissors and Paper Three pieces from one cut • Placing a strip on an edge • Charmed rings • Unexpected results of cutting • Paper chain • Thread yourself through a sheet of paper. Perhaps you think, as I once did, that there are some unnecessary things in this world. You’re quite mistaken: there is no junk that might not be of help sometime for some purpose. What is useless for one purpose, comes in handy for another, and what is useless for business might be suitable for leisure. In the corner of a room being repaired I once came across several used postcards and a heap of narrow paper strips that had been trimmed from wall paper. “Rubbish for the fire,” I thought. But it turned out that even with this junk one can interestingly amuse oneself. My elder brother Alex showed me some things you could do with them. He started with the paper strips. Giving me a piece of strip about 30 centimetres long, he said: “Take a pair of scissors and cut the strip in three...” I was about to cut but Alex stopped me: “Wait a bit, I haven’t finished yet. Cut it into three with one cut of the scissors.” This was more difficult. I tried one way and then another, and then began to think my brother had posed a virtually impossible problem. Eventually it occurred to me that it was absolutely intractable. “You’re pulling my leg,” I said, “It’s impossible.” “Well, think again, maybe you’ll work it out.” “I have worked it out that the problem has no solution.” “Too bad. Let me.” Brother took the strip, folded it in two and cut it in the middle to produce three pieces. “You see?” 3-621 By the Way “Yes, but you’ve folded the strip.” “Why didn’t you?” “You didn’t say I could.” “But I didn’t say you couldn’t either. Simply agree that you didn’t see the solution.” “All right. Give me another problem. You won’t catch me out again.” “Here is another strip, put it on its edge.” “So that it stands or falls?” I asked suspecting a trap. “Standing, of course. If it falls, it will mean that it was laid, not stood on edge.” “So that it stands... on its edge,” I muzed, and it suddenly occurred to me that I could bend the strip. I did so and put it on the table. “There, standing on its edge! You didn’t say I couldn’t bend it!” I said triumphantly. “Right.” “More of your problems, please.” “As you like. You see I’ve glued the ends of several strips and produced paper rings. Take a red-and-blue pencil and draw a blue line all along the outside of this ring and a red along the inside.” “And then?” “That’s all.” A silly job, but somehow it didn’t quite come off. When I had joined up the ends of the blue line and wanted to do the red, I found to my surprise I had absent-mindedly drawn the blue line on both sides of the ring. “Give me another,” I was embarrassed, “I’ve accidentally spoiled the first one.” But the second was a failure, too. I even didn’t notice how I had drawn the both sides. “Some delusion! Again. Give me another.” “You are welcome.” Well, what do you think? Again, both sides appeared blue! There was no room for the red. I was upset. “Such a simple thing and you can’t do it,” smiled brother. “Just look.” He took a paper ring and swiftly drew a red line all round the outside and a blue one on the inside. Having received a fresh ring, I started as carefully as possible to draw the line along one side, trying very hard not to go over to the other side somehow, and... joined up the line. Dear me! Both sides again. About to weep, I in bewilderment glanced at my brother, and only then I guessed from his grin that something was wrong. “Well, you just... Is it a trick?” I asked. “The rings are magic.” “What magic? Just rings. You’ve just fixed up something.” “Try to make something else with these rings. For example, can you cut this ring to get two thinner ones?” “Nothing special.” Having cut the ring, I was about to demonstrate two thin rings I had got when I noticed, much to my surprise, that I had in my hands only one long ring, not two smaller ones. “Okay, where are your two rings?” Alex asked mockingly. “Anotherphysical experiments, when treated attentively, can suggest fundamental ideas. These are those small things that teach us great ideas. Dry Out of Water You’ll now see that the air surrounding us on all sides exerts a significant pressure on all the things exposed to it. The experiment I’m going to describe will show you more vividly the existence of what physicists call “atmospheric pressure”. Place a coin (or metal button) on a flat plate and pour some water over it. The coin will be under water. It’s impossible, you are sure to think, to get it out from under the water with your bare hands without getting your fingers wet or removing the water from the plate. You’re mistaken, it is possible. Proceed as follows. Set fire to piece of paper inside a glass and when the air has heated, upend the glass and put it on the plate near the coin. Now watch, you 66-67 For Young Physicists won’t have to wait long. Of course, the paper under the glass will burn out soon and the air inside the glass will begin to cool down. As it does so, the water will, as it were, be sucked in by the glass and before long it will be all there, exposing the plate’s bottom. Wait a minute for the coin to dry and take it without wetting your fingers. The reason behind these phenomena is not difficult to understand. On heating, the air in the glass expanded, just as all bodies would do, and the extra amount of air came out of the glass. But when the remaining air began to cool down, its amount was no longer enough to exert its previous pressure, i.e. to balance out the external pressure of the atmosphere. Therefore, each square centimetre of the water under the glass was now subject to less pressure than the water in the exposed part of the plate and so no wonder it was forced under the glass by the extra pressure. In consequence, the water was not really “sucked in” by the glass, as it might seem, but pushed under the glass from the outside. Now that you know the explanation of the phenomenon in question, you will also understand that it is by no means necessary to use in the experiment a burning piece of paper or cotton wool soaked in alcohol (as is sometimes advised), or any flame in general. It suffices to rinse the glass with boiling water and the experiment will be as much of a success. The key thing here is to heat the air in the glass, no matter how that is done. The experiment can be performed simply in the following form. When you have finished your tea, pour a little tea into your saucer, turn your glass upside down while it is still hot, and stand it in the saucer and tea. In a minute or so the tea from the saucer will have gathered under the glass. Parachute Make a circle about a metre across out of a sheet of tissue-paper and then cut a circle a few centimetres wide in the middle. Tie strings to the edges of the large circle, passing them through small holes; tie the ends of the strings, which should be equally long, to a light weight. This completes the manufacture of a parachute, a scaled-down model of the huge umbrella that saves lives of airmen who, for some reason or other, are For Young Physicists compelled to escape from their aircraft. To test your miniature parachute in action drop it from a window in a high building, the weight down. The weight will pull on the strings, the paper circle will blossom out, and the parachute will fly down smoothly and land softly. This will occur in windless weather but on a windy day your parachute will be carried away however weak the wind and it will descend to the ground somewhere far from the starting point. The larger the “umbrella” of the parachute, the heavier the weight the parachute will carry (the weight is necessary for the parachute not to be overturned), the slower it will descend without a wind and the farther it will travel with a wind. But why should the parachute keep up in the air so long? Surely, you’ve guessed that the air stops the parachute from falling at once. If it were not (or the paper sheet, the weight would hit the ground quickly. The paper sheet increases the surface of the falling object, yet adding almost nothing to its total weight. The larger the surface of an object, the more drag there is on it. If you’ve got it right, you’ll understand why particles of dust are carried about by the air. It is widely believed that dust floats in air because it is lighter. Nonsense! What are particles of dust? Tiny pieces of stone, clay, metal, wood, coal, etc., etc. But all of these materials are hundreds and thousands of times heavier than air; stone, is 1,500 times heavier; iron, 6,000 times; wood, 300 times, and so on. A speck of solid or liquid should infailingly fall down through the air, it “sinks” in it. It does fall, only falling it behaves like a parachute does. The point is that for small specks the surface-to-weight ratio is larger than for large bodies. Stated another way, the particles’ surfaces are relatively large for their weight. If you were to compare a round piece of lead shot with a round bullet that is 1,000 times as heavy as the shot, the shot’s surface is only 100 times smaller than the bullet’s. This implies that the shot’s surface per unit weight is 10 times larger than the bullet’s. Imagine that the shot shrinks until it becomes one million times lighter than the bullet, that is, turns into a speck of lead. Its “specific” surface would be 10,000 times larger than the bullet’s. Accordingly, the air would hinder its motion 10,000 times more strongly than it does the bullet’s. 68-69 For Young Physicists Figure 42 That’s why it would hover in the air hardly falling and being carried by the slightest wind away and even upwards. A Snake and a Butterfly Cut a circle about the size of a glass hole from a postcard or a sheet of strong paper. Cut a spiral in it in the form of a coiled-up snake, as shown in Fig. 42. Make a small recess in the tail to receive a knitting-pin fixed upright. The coils of the snake will hang down forming sort of a spiral stairs. Now that the snake is ready, we can set out to experiment with it. Place it near a hot kitchen stove: the snake will spin and the faster, the hotter the stove. Near any hot object (a lamp or tea kettle, etc.) the snake will rotate while the object remains hot. So, the snake will spin very fast if suspended above a kerosene lamp from a piece of string. What makes the snake rotate? The same thing that makes the arms of a windmill rotate-the flow of air. Near every heated object, there is an air flow moving upwards. This flow occurs because air, just like any other material, expands on heating and becomes thinner, i.e. lighter. The surrounding air, which is colder and thus denser and heavier, displaces the hotter air, making it rise, and occupies its place. But the fresh portion of air heats at once and, just like the first one is ousted by a yet fresher amount of colder air. In this way, each heated object gives rise to an ascending flow of air around it, which is maintained all the time the object is warmer than the surrounding air. In other words, a barely noticeable warm wind blows upwards from every heated object. It strikes the coils of our paper snake making it rotate, just as wind makes the arms of a windmill rotate. Instead of a shake you can use a piece of paper in another shape, for example a butterfly. Cut it out of tissue-paper, bind in the middle and suspend from a piece of a very thin string or hair. Hang the butterfly above a lamp and it will rotate like a live one. Also, the butterfly will cast its shadow on the ceiling and the shadow will repeat the motions of the rotating paper butterfly magnified up. It’ll seem to an uninitiated person that a large black butterfly has flown into the room and is hectically hovers under the ceiling. You can also make as follows: strick a needle intoFor Young Physicists a cork and place the paper butterfly on the needle’s tip at the point of equilibrium which can be found by trial and error. The butterfly will rotate quickly if placed above a warm thing, in fact putting your palm under it will be enough for the butterfly to rotate. We come across the expansion of air as it heats and ascending warm currents everywhere. It is well known that the air in a heated room is the warmest near the ceiling and the coldest near the floor. That’s way it seems sometimes that there is a draught near our feet when the room hasn’t properly heated up. If you leave the door from a warm room to a colder one ajar, cold air will flow into the warm one along the floor and warm air will flow out along the ceiling. The flame of candle placed near the door will indicate the direction of these flows. If you want to keep the warmth in a heated room you should see to it that no cold air comes in from under the door. You need only to cover the gap by a rug or just a newspaper. Then the warm air won’t be ousted from below by the colder one and won’t leave the room through holes higher up in the room. And what is the draught in a furnace or a chimney stack but an ascending flow of warm air? We could also discuss the warm and cold flows in the atmosphere, trade winds, monsoons, breezes and the like but it would lead us too far astray. Ice in a Bottle Is it easy to get a bottle full of ice during the winter? It would seem that nothing could be easier when it is frosty outdoors. Just put a bottle of water outside the window and let the frost do the job. The frost will cool the water and you will have a bottleful of ice. But if you actually try to do the experiment, you’ll see that it is not that easy. You will obtain ice but the bottle will be destroyed in the process, it’ll burst under the pressure of the freezing water. This occurs because water, on freezing, expands markedly, by about a tenth of its volume. The expansion is so powerful that it bursts both a corked bottle and the bottleneck of an open bottle, the water frozen in the neck becomes, as it were, an ice cork. The expansion of freezing water can even break metal walls if they are not too thick. So, water can break the 5-cm walls of a steel bomb. No wonder that 70-71 For Young Physicists water pipes burst so often in winter. The expansion of water on freezing also accounts for the fact that ice floats on water and doesn’t sink. If water contracted on cooling, just like all other liquids do, then ice wouldn’t float on the water’s surface but would go down to the bottom. And those of us in northern countries wouldn’t enjoy skating and travelling on the ice of our rivers and lakes. To Cut Ice and... Leave It One Piece Figure 45 You may have heard that pieces of ice “freeze up” under pressure. This doesn’t mean that pieces of ice freeze up more strongly when exposed to pressure. On the contrary, under strong pressure ice melts, but once the cold water produced in the process is free of the pressure, it refreezes (as its temperature is below 0°C). When we compress pieces of ice, the following occurs. The ends of the parts that contact each other and are subject to high pressure melt, yielding water at a temperature below zero. This water fills in tiny interstices between the parts that are sticking out and when it is not subjected to the high pressure any more it freezes at once, thus soldering the pieces of ice into a solid block. You can test this by an elegant experiment. Get a beam of ice, and support its ends by the edges of two stools, chairs or the like. Make a loop of a thin steel wire 80 centimetres long and put it round the beam, the wire should be 0.5 millimetre or a little less thick. Finally, suspend something heavy (about 10 kilogrammes) from the ends of the wire. Under the pressure of the heavy object the wire will bite into the ice and cut slowly through the whole of the beam but... the beam will still remain one piece. You may safely take it in your hands as it will be intact as if it had not been cut! After you’ve learned about the freezing up of ice, you’ll see why it works. Under the thrust of the wire the ice melted but the water flowed over the wire and free of the pressure refroze at once. In plain English, while the wire cut the lower layers, the upper layers were freezing again. Ice is the only material in nature with which you can do this experiment. It’s for this reason that we can skate and toboggan over ice. When a skater presses all his weight on his skates, the ice melts under the For Young Physicists pressure (if the frost is not too severe) and the skate slides along where it again melts some ice and the process occurs continuously. Wherever the skate goes a thin layer of ice turns into water that when free of the pressure refreezes. Therefore, although the temperature might be below freezing point, the ice is always “lubricated” with water under skates. That’s why it’s so slippery. Sound Transmission You may have observed from a distance a man using an axe or a carpenter driving in nails. You may then have noticed an unusual thing, you do not hear the stroke when the axe touches the tree or when the hammer hits a nail, but you hear it later when the axe (or hammer) is ready for the next stroke. Next time you happen to observe something similar, move a little forward or backward. After trying several times you’ll find a place where the sound of a stroke comes just at the moment of a visible stroke. Then return to where you started and you’ll again notice the lack of coincidence between the sound and the visible stroke. Now it should be easy for you to guess the reason behind this enigmatic phenomenon. Sound takes some time to cover the distance from the place where it originated to your ear; on the other hand, light does it nearly instantaneously. And it may happen that while the sound is travelling through the air to your ear, the axe (or hammer) will have been raised for a new stroke. Then your eyes will see what your ears hear and it’ll seem to you that the sound comes when the tool is up and not when the tool is down. But if you move in either direction just a distance, covered by the sound during a swing of the axe, then by the time the sound reaches your ear the axe will strike again. Now, of course, you’ll see and hear a stroke simultaneously, only it’ll be different strokes since you’ll hear an earlier stroke, perhaps the last but one or even earlier. What is the distance covered by sound in one second? It has been measured exactly, but approxi¬ mately it is about 1/3 of a kilometre. So sound covers one kilometre in 3 seconds, and if the wood-cutter swings his axe twice a second, you’ll have to be 160 metres away for the sound to coincide with the axe as he raises it. But light travels each second in air almost 72-73 For Young Physicists a million times as far as sound. So you can understand that for any distances on earth we can safely take the speed of light to be infinite. Sound is transmitted not only through the air but also through other gases, liquids and solids. So in water, sound travels four times faster than in air, and under water sound can be heard distinctly. People working in underwater caissons can hear sounds from the shore perfectly and anglers will tell you how fish scatter at the slightest suspicious noise from the shore. Elastic solids are better still as sound transmitters, e. g. cast iron, wood, and bone. Put your ear to the end face of a long wood beam or a block and ask somebody to tap it slightly at the other end. You’ll hear the dull sound of the stroke transmitted through the entire length of the beam. If it’s rather quiet and spurious noises don’t interfere, you can even hear a clock ticking at the opposite end of your beam. Sound is transmitted equally wellalong iron rails or beams, cast iron tubes, and even soil. If you put your ear to the ground you can hear the clatter of horses’ hoofs long before the sound comes through the air and in this way you can hear thunder that is so far away that no sound comes to you by air at all. Only elastic solids transmit sound so well, soft tissues and loose, inelastic materials are very poor sound transmitters since these “absorb” it. That’s why they hang thick curtains near doors if they don’t want any sound to reach an adjacent room. Carpets, soft furni¬ ture and clothes have the same effect on sound. Figure 46 A Bell Among the materials distinguished for their perfect sound transmission I’ve mentioned bones. Do you want to make sure that the bones of your skull have this property? Hold the ring of a pocket watch with your teeth and close your ears with your hands. You’ll still quite distinctly “hear” the measured strokes of the balance, and they’ll be louder than the ticking perceived through the ear. This sound comes to your ears through the bones of your skull. A further fascinating experiment testifying to the good transmission of sound through your skull. Tie a soup spoon in the middle of a piece of string so that the string has two loose ends. Press these ends with your fingers to your closed ears and, leaning forward For Young Physicists for the spoon to swing freely, make it strike something solid. You’ll hear a low-pitched drone as if a bell is ringing near your ears. The experiment comes out better if you use something heavier instead of the spoon. A Frightening Shadow One evening my brother Alex asked, “Want to see something unusual? Come into this room.” The room was dark. Alex took a candle and we walked in. I led the way and so was the first to enter the room. But suddenly I was stunned: an incongruous monster eyed me from the wall. Flat as a shadow, it stared at me. To tell the truth, I got a little frightened. I might have taken to my heels had it not been for my brother’s laughter behind me. I turned round and saw the reason. There was a mirror on the wall covered with a sheet of paper that had eyes, a nose, and a mouth cut in it. Alex had so directed the candle’s light that these parts of the mirror reflected directly onto my shadow. Thus, I was scared by my own shadow. But later, when I attempted to play this joke on my friends, it turned out that arranging the mirror properly is not that easy. It took a lot of practice to master the art. Light rays are reflected in a mirror according to the following rule: the angle at which light rays strike the mirror equals the angle at which they are reflected. After I’d learned the rule it was no problem to work out where to locate the candle with respect to the mirror for the light spots to be cast at the required place on the shadow. 74-75 For Young Physicists To Measure Light Brightness At twice the distance, clearly, a candle illuminates much weaker. But how many times weaker? Two? No, if you place two candles at double the distance, you won’t obtain the previous illumination. In order to obtain the earlier illumination at double the distance you’d have to put two times two, i.e. four candles, not two. At triple the distance you’d need three times three, i.e. nine candles, not three, and so forth. It follows that at twice the distance illumination is four times weaker; at three times the distance, nine times weaker; at four times the distance, 16 times; and at five times the distance, 5 x 5 or 25 times weaker, and so on. This is the law of weakening illumination with distance. Note in passing that this is also the law of sound attenuation with distance. For example, sound attenuates on six times the original distance by 36 times, not by 6 times’". Knowing this law we can make use of it to compare the brightness of two lamps, or any two light sources in general. For instance, you wish to compare the brightness of your lamp with that of a conventional candle, in other words, you want to find out how many candles you need to replace the lamp to obtain the same illumination. For this purpose place the lamp and a burning candle at one end of a table and at the other you stand a sheet of white cardboard clamped between books as Figure 48 * This explains why a whisper from your neighbour drowns the loud voice of an actor on the stage in a theatre. If the actor is only 10 times farther away from you than your neighbour, then the actor’s voice is attenuated 100 times more than what you’d hear if the same sound came to you from the lips of your neighbour. It’s not surprising then that for you the actor’s voice is weaker than the whisper. For exactly the same reason it’s important for students to keep quiet when the teacher speaks. The teacher’s words reaching students (especially those far away) are so attenuated that even a soft whisper from a neighbour will muffle them completely. For Young Physicists shown. Just in front of the sheet fix up a stick, e.g. a pencil, also upright. It will cast two shadows onto the cardboard, one from the lamp and the other from the candle. The density of the two shadows is, generally speaking, different because both are lit, one by the bright lamp, the other by the dimmer candle. By bringing the candle nearer you can achieve a situation in which both shadows will have the same “blackness”. This will mean that the illumination due to the lamp just equals that due to the candle. But the lamp is far¬ ther away from the cardboard than the candle. Measuring how many times farther away will tell you how many times the lamp is brighter than the candle. If, say, the lamp is three times farther away from the cardboard than the candle, then its brightness is 3 x 3, i.e. nine times the brightness of the candle. Remember the law? Another way of comparing the luminous intensity of two sources relies on the use of an oil spot on a sheet of paper. The spot will seem light if illuminated from behind, and dark if lit from the front. So the sources to be compared can be placed at such distances that the spot will seem equally illuminated on either side. Then it only remains to measure the respective distances and repeat the previous process. And in order that both sides of the spot might be compared it is a good idea to place the paper near a mirror, you should know how. Upside Down If your home has a room facing south, you could easily make it into a physical device that has an old Latin name camera obscura. You’ll have to close the window with a shield, made of a plywood or cardboard glued with dark paper with a small hole made in it. On a fine sunny day close the doors and windows to darken the room and place a large sheet of paper or a sheet opposite the hole. This will be your “screen”. You’ll immediately see on it a reduced image of what can be 76-77 For Young Physicists seen from the room through the hole. Houses, trees, animals, and people, everything will appear on the screen in its natural colours, but... upside down. What does this experiment prove? That light propagates in straight lines. The rays from the upper and lower parts of an object cross in the hole and travel on so that now the top rays appear below and the bottom rays above. If the rays were not straight but curved or broken, you’d have got something different. Significantly, the shape of the hole has no effect whatsoever on the image. You might drill a round hole, or make a square, triangular, hexagonal, or other hole-the image on the screen would be the same. Did you happen to observe oval light circles under a dense tree? These are nothing but images of the Sun painted by the rays that pass through various gaps between the leaves. The images are roundish because the sun is round, and elongated because the rays are obliquely incident on the ground. Put a sheet of paper atright angles to the solar rays and you’ll obtain round spots on it. During solar eclipses when the dark sphere of the moon blots out the sun leaving only a bright crescent, the small spots under trees turn into small crescents as well. The old photographer’s camera, too, is nothing but a camera obscura, the only difference being that at the hole an objective lens is fitted for the image to be brighter and clearer. The back wall is a frosted glass on which the image is produced, upside down of course. The photographer can only view it if he covers himself and the camera by a dark cloth to keep out any spurious light. You can make a simple model of this sort of camera. Find a closed elongated box and drill a hole through one wall. Remove the wall opposite the hole and stretch over the gap an oiled piece of paper instead-a substitute for the frosted glass. Bring the box into our dark room and place it so that its hole is just opposite the hole in the darkened window. On the back side you’ll see a distinct image of the outside, again upside down of course. Your camera is convenient in that you no longer need a dark room and you can bring it out into the open and put it where it suits you. You’ll only need to cover your head and the camera with a dark cloth for the spurious light not to interfere. For Young Physicists Overturned Pin We have just discussed the camera obscura and a way of manufacturing it but we omitted one interesting thing: every human being always has a pair of small cameras like that about him or her. These are our eyes. Just fancy, your eye is just like the box that you were shown how to make above. What we call the pupil of the eye is not a black circle on the eye but a hole leading into the inside of your organ of sight. The hole is covered with a transparent envelope on the outside and with a jelly-like and transparent substance underneath. Next to the pupil behind it is the crystalline lens having the form of a convexo-convex glass, and the inner cavity of the eye between the crystalline lens and the back wall, on which the image is produced, is filled with a transparent substance. A cross section through the eye is given in Fig. 50. Despite all these distinctions the eye is still a camera obscura, only an improved one, as the eye produces high-quality, distinct images. The images at the back of the eye are minute. So, an 8-m high lamp-post seen 20 metres away from the eye is only a tiny line, about 5 millimetres long, at the back of the eye. But the most interesting thing here is that although all the images are upside down, we perceive them as they are. This turning over is due to long habit. We are used to seeing with our eyes so that each visual image obtained is converted into its natural position. That this is really true, you could test by an experiment. We’ll attempt to contrive it so that we get at the back of the eye not an inverted, but direct image of an object. What will we see then? Since we are used to inverting every visual image, we’ll invert this one as well. Accordingly, we’ll in this case too see an inverted image, not a direct one. In actual fact that is exactly what happens and the following experiment will demonstrate it in a fairly graphic manner. Make a pinhole in a postcard and hold it against a window or a lamp about 10 centimetres away from your right eye. Hold the pin between you and the postcard so that its head is opposite the hole. With this arrangement you’ll see the pin as if it were behind the hole, and what is of the more importance here, upside down. This unusual situation is presented in Fig. 51. Move the pin to the right and your eyes will tell you it’s moved to the left. 78-79 For Young Physicists The explanation is that the pin at the back of your eye is here depicted not upside down but directly. The hole in the card plays the role of a light source producing the shadow of the pin. The shadow falls on the pupil and its image is not inverted as it’s too close to the pupil. On the back wall of the eye a light spot is produced-the image of the hole in the card. On it the dark silhouette of the pin is seen which is its shadow, the right way up. But it seems to us that through the hole in the card we see the pin behind the card (as only the part of the pin that gets in the hole is seen) and inverted at that because our eyes are in the habit of turning images upside down. Igniting with Ice When a boy, I liked watching my brother lighting a cigarette with a magnifying glass. He would put the glass in the sunlight and train the spot of light on the cigarette end. After a while it would begin to give off a bluish smoke and smolder. One winter day Alex said, “You know, it’s possible to light a cigarette with ice, too.” “With ice?” “Ice doesn’t ignite it, of course, the sun does. Ice only collects solar rays, just like this glass.” “So you want to make a magnifying glass out of ice?” “I can’t make glass of ice, nobody can, but we could make a burning lens from ice.” “What’s a lens?” “We’ll shape a piece of ice like this glass and it will be a lens: round and convex which means thick in the middle and thin at the edges.” “And will it ignite things?” “Yes.” “But it’s cold!” “What of it? Let’s try.” To begin with, my brother told me to fetch a washing basin. When I did he rejected it: “Nothing doing. You see, the bottom is flat. We need a curved bottom.” When I brought a suitable basin, Alex poured some clean water into it and put it outside, the temperature outdoors being below freezing point. “Let it freeze down to the bottom. We’ll then have an ice lens with one side flat and the other convex.” For Young Physicists Figure 52 Figure 53 “So big?” “The bigger, the better, it’ll catch more sunlight.” First thing in the morning I ran to inspect our basin. The water had frozen right through to the bottom. “What a good lens we’ll have,” Alex said tapping the ice with finger. “Let’s take it out of the basin.” This turned out to be no problem. Alex put the icy basin into another one containing hot water and the ice at the walls melted quickly. We got the ice basin out into the yard and placed the lens on a board. “Good weather, ins’t it!” Alex screwed up his eyes in the sunlight, “Ideal for igniting. Just hold the cigarette.” I did so and my brother, taking hold of the lens with both hands turned it towards the sun but so that he wasn’t in the way of the rays himself. He took aim painstakingly but eventually succeeded in training the lightspot directly on the end of the cigarette. When the spot rested on my hand, I felt it was hot and already I had no doubt that the ice would light the cigarette. Indeed, when the spot got onto the end of the cigarette and had stayed there for about a minute, the tobacco smoldered and discharged some bluish smoke. My brother took a puff at the cigarette, “Here you are, we’ve lit it with ice. In this way you could make a fire without matches even at the pole, if only you had firewood.” Magnetic Needle You can already make a needle float on the surface of water. Here you’ll have to use your skill in a new and more impressive experiment. Find a magnet, if only a small horse-shoe one. If you bring it near the saucer with a needle floating in it, the needle will obediently approach the appropriate edge of the saucer. The effect will be more noticeable, if before placing the needle on the water you pass the magnet several times along it (but only use one end of the magnet in one direction only). This turns the needle itself into a magnet, there¬ fore it’ll even approach a nonmagnetized iron object. You can make many curious observations with the magnetic needle. Leave it alone without attracting it by a piece of iron or the magnet and it’ll orient itself in the water in one direction, namely north-south, just like the needleof a compass. Turn the saucer and the needle will still point to the north with one end and to the south with the other. Bring one end (pole) of the 80-81 Figure 54 Figure 55 For Young Physicists magnet to an end of the needle and you’ll find that it won’t be attracted to the magnet at that end. It may turn away from the magnet in order that the opposite end might approach. This is a case of an interaction between two magnets. The law of this interaction states that unlike ends (the north pole of one magnet and the south pole of another) are attracted and like ones (both north or south) are repelled. Having investigated the behaviour of the magnetized needle, make a toy paper boat and hide your needle in its folds. You might astonish your uninitiated friends by controlling the motion of the boat without so much as touching it: it would obey every motion of your hand. Of course, you would be holding the magnet so that the spectators wouldn’t suspect it. Magnetic Theatre Or rather circus, as starring in it are rope dancers cut out of paper (of course). First of all, you have to make the circus building out of cardboard. At the bottom of it you’ll stretch a wire and fix above the stage a horse-shoe magnet, as shown. Now to the artists. They are cut out of paper, their stance being chosen to suit the purpose. The only condition is that their height be equal to the length of a needle glued on from behind along the length of the figure. You could use two or three drops of sealing-wax for the glue. If a figure like this is installed onto the “rope”, it not only won’t fall, but will stay upright pulled by the magnet. By slightly jerking the wire you’ll animate your rope dancers. They’ll swing and jump all the while keeping their balance. 6-621 For Young Physicists Electrified Comb Even if you’re ignorant of electricity and not even acquainted with its ABC, you can still do a number of electrical experiments that would be fascinating and will, in any case, be useful when you meet this amazing force of nature in future. The best place for these electrical experiments is a warm room in a frosty winter. These experiments are especially successful in dry air, and in winter warm air is far drier than air at the same temperature during summer. Now, to our experiments. You may have passed a conventional comb over dry (completely dry) hair. If you did so in a warm room in full silence, you may have heard some slight crackling on the comb. Your comb had been electrified by friction with the hair. The comb can also be electrified by material other than hair. If you rub it against a dry woollen fabric (a piece of flannel, say) it also acquires electrical properties and to quite a larger degree. These properties manifest themselves in a wide variety of ways, notably by attracting light objects. Bring a rubbed comb close to some pieces of paper, chaff, a ball of elder core, etc. and these small things will all stick to the comb. Make tiny ships of light paper and launch them on water. You’ll be able to control the movements of your paper fleet using an electrified comb like a magic wand. You could stage the experiment in a more impressive way. Place an egg in a dry egg-support and balance a rather long ruler on it. As the electrified comb approaches one of its ends the ruler will turn fairly quickly. You can make it follow the comb obediently moving it in any direction and making it rotate. An Obedient Egg Electrical behaviour is inherent not only in the comb but in other things as well. A rod of sealing-wax rubbed against a piece of flannel or the sleeve of your coat, if it’s woollen, behaves in the same way. A glass rod or tube, too, is electrified if rubbed by silk. But the experiment with silk is only a success in exceedingly dry air and only then if both the silk and the glass are well dried by heating. Here is a further funny experiment on electrical attraction. Empty a chicken egg through a small hole. 82-83 Figure 57 For Young Physicists which is best done by blowing the contents out through another hole at the opposite end. You’ve thus obtained an empty shell (the holes are sealed with wax). Put it on a smooth table, board or large plate and, using the electrified rod, make the empty egg roll obediently after it. An outsider, not aware that the egg is empty, would O be bewildered by experiment (invented by the English scientist Faraday). A paper ring or a light ball, too, follow an electrified rod. Figure 58 Interaction Mechanics teaches that one-sided attraction, or any one-sided action, in general, doesn’t exist. Any action is, in fact, an interaction. In consequence, if the electrified rod attracts various things, then it itself is attracted to them. To bear this out you have only to make the comb, or rod, easily movable, e.g. by suspending it from a loop made of a piece of thread (the thread should preferably be a silk one). Then, you will quickly find that any electrified thing- your hand, say-attracts the comb making it turn, and so forth. To repeat, this is a general law of nature. It shows up always and everywhere-any action is an interaction of two bodies affecting each other in opposite directions. Nature doesn’t know of an action that is one-sided and doesn’t involve the interaction of another body. Electrical Repulsion Let’s return to the experiment with the suspended electrified comb. We’ve seen that it is attracted by any electrified body. It would be of interest to test the way in which another, also electrified, thing affects it. An experiment will convince you that two electrified bodies can interact in different ways. If you bring an electrified glass rod to the electrified comb, the two things will attract each other. But if you bring an electrified sealing-wax rod or another comb to the comb, the interaction will be repulsive. The physical law describing this fact of nature states: unlike charges attract, like charges repel. Like charges 6* For Young Physicists Figure 59 Figure 60 will be those on plastics and sealing-wax (the so-called amber or negative, charge) and unlike charges are those on amber and glass which is positive. The ancient names “amber” and “glass” charges have now gone out to use, being completely replaced by the names “negative” and “positive” charges. The repulsion of like-charged things lies at the basis of a simple device to detect electricity-the so-called electroscope. The word “scope” comes from Greek and means to “indicate”, it enters words like “telescope”, “microscope”, and so forth. You can make this simple device on your own. Through the middle of a cardboard circle or a cork that fits the neck of a jar or bottle, a rod is passed, part of it protruding from the top. To the end of the rod two strips of foil or tissue-paper are attached using wax. Next the neck is plugged with the cork or cardboard circle, sealing the edges with sealing wax. The electroscope is ready to use. If now you bring an electrified thing to the protruding end of the rod, the two strips will become electrified, too. They charge up simultaneously and, therefore, separate due to electrostatic repulsion. The separation of the strips is the indication that the thing that touched the electroscope rod is electrified. If you are no good at handiwork, you could make a simpler version of the device. It won’t be as convenient and sensitive, but will still work. Suspend two elder-core balls on a stick from pieces of string so that they hang in contact with each other. That’s all. On touching a ball with a thing being tested you’ll notice that the other ball deflects if the thing is charged. Finally, in the accompanying figure you can see yet another form of a primitive electroscope. A foil strip, folded in two, is suspended from a pin stuck into a cork. Touching the pin with an electrifiedthing makes the strips separate. One Characteristic of Electricity With the help of an easily manufactured makeshift device you can observe the interesting and very important feature of electricity-to accumulate on the surface of an object only, and on protruding parts at that. Cement a match vertically to a match box using a sealing-wax drop, then make another such support. 84-85 For Young Physicists Now cut out a paper strip about a match-length wide and three match-lengths long. Turn the ends of the paper strip into a tube so that you could fix it to the supports. Glue three or four narrow ribbons of thin paper-tissue to the either side of the strip (Fig. 61) and fix the assembly on the matches. Our device is ready for experiments. Touch the straight strip with an electrified sealing-wax rod and the paper and all the ribbons on it will charge up simultaneously. This can be judged by the ribbons sticking out on either side. Now arrange the supports so that the strip curves into an arc, and charge it up. The strips will now stick out on the convex side only, those on the concave one will dangle as before. What does this indicate? That the electric charge has only accumulated on the convex side. If you make the strip into an S-shape, you’ll see that the electric charge is only present on the convex parts of the paper. A Sheet of Newspaper What is to “Look with Your Mind”? • Heavy Newspaper “Agreed. This evening we are performing electrical experiments,” my brother proclaimed tapping the tiles of the warm stove. I was delighted, “Experiments? New experiments! When? Right now? I’d like to now!” “Patience, my friend. The experiments will be this evening. Now I must be off.” “To get the machine?” “What machine?” “Electric. We’ll need a machine for our experiments.” “The machine that we’ll need is already available, it’s in my bag... And don’t you dare delve in there while I’m away,” Alex had read my thoughts. He went on to say, putting his coat on, “You’ll find nothing, and will only make a mess.” “But the machine is there?” “There, don’t worry.” My brother went out, carelessly leaving the bag with the machine in on a small table in the hall. If iron could feel, it would feel near a magnet exactly what I was feeling left alone with my brother’s bag. The bag was pulling me, attracting all my feelings and thoughts. It was absolutely impossible to think about something different or divert my eyes from the bag... It’s so strange that an electric machine can go inside a bag. I did not imagine it to be that flat. The bag wasn’t locked and I carefully peaped inside... Something wrapped in newspaper. A small box? No, books. Books? Only books, nothing more in the bag? I should have understood at once Alex was joking: how can you possibly hide an electric machine in a bag! Alex came back with empty hands and guessed at once the reason for my sorrowful looks. “We seem to have visited the bag don’t we?” he said. “Where is the machine?” I answered with a question. “In the bag, didn’t you see?” “There are only books in there.” “And the machine! You didn’t look very far. What did you look with?” “With what? Why, with my eyes?” “That’s just it, with your eyes. You didn’t use your brains. It’s not enough just to look, you have to understand what you see. That is called looking with your mind.” 86-87 A Sheet of Newspaper Figure 62 “How do you look with your mind?” “Do you want me to show to you the difference between looking with your eyes and looking with the whole of your head?” My brother produced a pencil and drew a figure (Fig. 62) on a sheet of paper. “The double lines here are railways, the single ones-highways. Take a look and say which of the railways is longer, the one from 1 to 2 or from 1 to 3?” “From 1 to 3, of course.” “You see it with your eyes. But now look at the figure with the whole of your head.” “But how? I can’t.” “Like this. Imagine that a straight line is drawn from 1 at a right angle to the lower highway 2-3,” my brother drew a dash line in his drawing. “How will my line separate the highways? Into what parts?” “In two.” “Exactly. This implies that all the points of this dash line are equidistant from 2 and 3. What will you say now about point I? Is it closer to 2 or 3?” “Now I see that it’s the same distance from 2 and 3. But earlier it seemed that the right-hand railway was longer than the left.” “Earlier you only looked with your eyes, but now you’re using your head. See the difference?” “I see. But where’s the machine?” “What machine? Oh, yes, the electric machine. In the bag. It’s still there. You didn’t notice because you didn’t look with your mind.” My brother took a bundle of books out of the bag, carefully unwrapped it from a large newspaper sheet and gave it to me. “Here’s our electric machine.” I looked at the newspaper in bewilderment. “Do you think it’s only paper and nothing more?” My brother went on to say, “According to your eyes, yes. But someone who can use his brains will perceive a physical device in this paper.” “Physical device? To make experiments?” “Yes. Hold the newspaper in your hands. It’s light, isn’t it? And, of course, you’ll think that you can always lift it even with a single finger. But now you’ll see that this very newspaper can at times be very heavy. Give me that ruler.” “It’s got serrated and isn’t good for anything.” “All the better, it doesn’t matter if it gets broken.” A Sheet of Newspaper Alex put the ruler on a table so that a part of it overhung the edge. “Touch the protruding end. It’s easy to press it down, isn’t it? Well, try to press it down after I’ve covered the other end with the newspaper.” He spread the newspaper on the table over the ruler, carefully smoothing the folds. “Now take a stick and strike the protruding part of the ruler very hard. Strike with all you strength!” I swung the stick back, and said, “I’ll strike it so hard that the ruler will break through the paper and hit the ceiling!” “Go ahead, don’t spare your strength.” The result was astonishing: there was a crack, the ruler broke, but the newspaper remained on the table, still covering the other piece of the ruler. Alex asked archly, “The newspaper appears to be heavier than you’ve been thinking?” Bewildered, I shifted the eyes from the fragment of the ruler to the newspaper. “Is it an experiment? Electric?” “It’s an experiment but not electric one. The electric ones will follow. I just wanted to show you that a newspaper can actually be a device to do physical experiments with.” “But why didn’t it let the ruler go? Look, I can easily lift it from the table.” That is the kernel of the experiment. Air presses down on the ruler with a powerful force: a good solid kilogramme on each centimetre of the newspaper. When you strike the protruding end of the ruler, its other end pushes up against the newspaper from below, and so the newspaper should rise. If it’s done slowly some air gets under the rising paper and compensates for the pressure from above. But your stroke was so fast that air had no time to get under the paper. Thus the edges of the paper were still sticking to the table when its middle was already being forced upwards. Therefore, you had to lift not only the paper but also 88-89 A Sheet of Newspaper the paper with the air pressing down on it. In a nut¬ shell, you had to lift with the ruler as many kilogrammes as there were square centimetres in the newspaper. If it were an area of only 16 square centimetres (a square with a side of 4 centimetres), then the air pressure would be 16 kilogrammes. But the area you lifted was notably larger, and accordingly, you had to lift a substantial weight, perhaps something near 50 kilogrammes. The ruler couldn’t bare this load and broke. Now do you believe that a newspaper can be used for physicalexperiments? After dark, we’ll make the experiments.” Sparks from Fingers • Obedient Stick • Electricity in Mountains My brother took a clothes-brush in one hand and held the newspaper against the warm stove with the other. He then began to rub the newspaper with the brush like a decorator smoothing wall-paper on the wall for the paper stick perfectly. “Look!” Alex said and took both hands away from the paper. I had expected that the paper would slide down onto the floor. This, however, didn’t happen: strange as it was, the paper stuck to the smooth tiles as if glued. I asked, “How does it keep on? It’s not smeared with glue.” “The paper is held by electricity. It’s now electrified and attracted to the stove.” “Why didn’t you tell me that the newspaper in the bag was electrified?” “It wasn’t. I did it right now, before your eyes, by rubbing it with the brush. The friction electrified it.” “So, it’s a real electric experiment?” “Yes, but we’re just beginning... Turn off the lights please.” In the dark the black figure of my brother and the greyish spot of the stove looked blurred. “Now watch my hand.” I guessed, rather than saw what he did. He took the paper down from the stove and, holding it with one hand, moved his spread fingers of the other hand to it. And then-I could hardly believe my eyes-sparks flew out from his fingers, bluish-white sparks! ‘The sparks were electricity. Want to try for your¬ self?” A Sheet of Newspaper I promptly hid my hands behind the back. Not for the world! My brother again applied the paper to the stove, brushed it and again produced an avalanche of long sparks from his fingers. I managed to notice that he didn’t touch the newspaper at all, but held his fingers about 10 centimetres away from it. “Don’t be scared, just try, it doesn’t hurt. Give me your hand,” he took hold of my hand and led me to the stove. “Spread your fingers!.. Well! Does it hurt?” In a twinkling of an eye a bundle of bluish sparks shot out from my fingers. In their light I saw that my brother had only partially detached the newspaper from the stove, the lower part being still “glued”. Simultane¬ ously with the sparks I felt a slight prick but the pain was trifling. Indeed, nothing to be scared of. “Again!” I asked. Alex applied the newspaper to the stove and began to rub, this time only with his palms. “What are you doing? Have you forgotten the brush?” “It’s all the same. Now, are you ready?” “Nothing doing! You’ve rubbed it with bare hands without using the brush.” “It’s possible without the brush too if only your hands are dry. You just have to rub.” And it was true, this time also sparks rained from my fingers. After I had the sparks to my heart’s content my brother proclaimed: “That’ll do. Now I am going to show you a flow of electricity, just like the one Columbus and Magellan saw at the tops of the masts of their ships... Pass me the scissors.” In the dark Alex brought the points of the spread scissors near to the newspaper, which was half- separated from the stove. I expected to see sparks but saw something new, the points of the scissors were crowned by glowing bundles of short bluish and reddish threads although the scissors were still far away from the paper. This was accompanied by faint prolonged hissing. “Sailors often see the same sort of fire brushes, only far larger ones, at the mastheads and yardarms. They called them St. Elm’s fires.” “Where do they come from?” “You mean who holds an electrified newspaper above the masts? True, there’s no newspaper there, but a low 90-91 A Sheer of Newspaper electrified cloud. It’s a substitute for the newspaper. You shouldn’t think, however, that this sort of electric glow on pointed structures only occurs at sea, it’s also observed on land, especially in the mountains. So, Julius Caesar wrote that on a night in a cloudy weather the spear heads of his legionnaires glowed this way. Sailors and soldiers are not afraid of these electric lights - on the contrary they view them as a good omen. Of course, without any reasonable grounds. In the mountains electric glows even occur on people at times, on their hair, caps, ears-that is, on all the protruding parts. In the process, they often hear a buzz, like the one produced by our scissors.” “Does this fire burn strongly?” "Not at all. After all, this isn’t a fire, but a glow, just a cold glow. So cold and harmless that it cannot even ignite a match. Look: instead of the scissors I use a match. And you see: the head is surrounded by the electric glow, but it doesn’t go off.” “But I think it is burning because flames are coming out straight from the head.” “Turn on the light and inspect the match.” I made sure that the match not only hadn’t charred but it hadn't even blacken. It was thus indeed sur¬ rounded by a cold light, and not fire. “Leave the light on. We’ll carry out the next experiment in the light.” Alex shifted a chair to the middle of the room and put a stick across its back. After several tries he managed to balance the stick at one point. “I didn't know that a stick could be supported in this way,” I said, “it’s so long.” “It works for exactly that reason. A short one wouldn’t. A pencil, for example.” I agreed, “A pencil, no means.” “Now, to business. Can you make the stick turn towards you without touching it?” I thought about it. “If we loop a rope onto its end...” I began. “No ropes, it must touch nothing. Can you?” “Aha, insight!” I put my face close to the stick and began sucking air into my mouth to attract the stick to me. It didn’t stir, however. “Any progress?” “None. It’s impossible!” A Sheet of Newspaper Figure 67 “Impossible? Let’s see.” He took the newspaper, down from the stove, where that had been sticking to the tiles, and began slowly to move it sidewards towards the stick. At about half a metre away the stick “felt” the attraction of the electrified newspaper and obediently turned in its direction. By moving the newspaper Alex made the stick follow it rotating at the back of the chair, first in one direction, then in the other. “The electrified newspaper, you see, attracts the stick so strongly that it follows and will follow the paper until all the electricity has flowed from the newspaper into the air.” “It’s a pity that these experiments cannot be performed in the summer-the stove will be cold.” “The stove is only necessary to dry up the paper since these experiments are only a success with an absolutely dry newspaper. You may have noticed that newspapers absorb moisture from the air and therefore are always somewhat damp, that’s why it has to be dried. You shouldn’t think, however, that in summer our experiments are impossible. They can be done but not so well as in winter when the air in a heated-up room drier than in summer-that’s the reason. Dryness is crucial for these experiments. In summer, a newspaper can be dried with a kitchen stove when it’s not too hot for the paper not to ignite on it. After the paper has been dried adequately, it’s brought onto a dry table and rubbed hard with a brush. The paper electrifies, but not as with a tile stove... Well, let’s call it a day. Tomorrow we’ll do some new experiments.” “Also electric?” “Yes, and with the same electric machine, our newspaper. Meanwhile I’ll give you an interesting account of Elm’s fires by the famous French naturalist Saussure. In 1867 he with several companions climbed the Sarley Mountain, which is more than 3 kilometres high. And here’s what they experienced there. Alex took down the book The Atmosphere by Flammarion from the bookcase, thumbed through it and gave me the following passage to read: “The climbers leaned their alpenstocks against a cliff and were preparing for their dinner when Saussure felt a pain in his shoulders and back as if a needle were beingdriven slowly into his body. ‘Thinking some pins had got into my canvas cape,’ recounted Saussure, ‘I threw it off but there was no relief, on the contrary, the 92-93 A Sheet of Newspaper pain became more accute and embraced the whole of my back from shoulder to shoulder. It was as if a wasp was walking all over my skin stinging it everywhere. I hastily threw off another coat but I could find nothing that could hurt so badly. The pain continued and came to feel like a burn. It seemed to me that my woollen sweater had caught fire and I was about to undress when my attention was attracted by a noise, a sort of hum. It came from the alpenstocks we had leaned against the cliff and resembled the rumbling of heated water about to boil. The noise continued for five minutes or so. ‘I then understood that the painful sensation was caused by an electrical flux released by the mountain. In the broad daylight I didn’t see any glow on the alpenstocks. They produced the same sharp noise whether they were held vertically with the tip pointed up and down, or horizontally. No sound came from the soil. ‘In several minutes I felt that the hair on my head and beard were rising as if a dry razor was being passed over a stiff beard. My young companion cried out that the hair of his moustache was rising and the tops of his ears were giving off strong currents. Having raised my hands, I felt currents emanating from my fingers. In short, electricity was being liberated from sticks, clothing, ears, hair, in fact everything that was protruding. ‘We left the summit hastily and descended about a hundred metres. As we were climbing down, our alpenstocks were producing ever lower noise and finally, the sound became so soft that we could only hear it by bringing them close to our ears.’” In the same book I read about other cases of Elm’s fires. “The liberation of electricity by protruding rocks is often observed when the sky is covered by low clouds gliding just over summits. “On June 10, 1863, Watson and several tourists climbed up the Jungfrau pass in Switzerland. It was a fine morning but the travellers got into a strong hail storm in the pass. A terrible clap of thunder came and soon Watson heard a hissing sound coming from his stick that resembled the sound of a kettle about to boil. The people stopped and found that their sticks and axes produced the same sound, and didn’t stop making the sound even when stuck with one end into the A Sheet of Newspaper Figure 68 ground. One of the guides took his hat off and cried that his head was burning. His hair stood on end as if electrified and everybody had tickling feelings on the face and other parts of the body. Watson’s hair straightened out completely. The stirring of fingers in the air produced electric hiss from their tips.” Dance of Paper Buffoons • Snakes • Hair on End Alex kept his word. Next day after dark he resumed the experiments. First of all he “glued” the newspaper to the stove. Then he asked me to get him paper denser than newspaper, writing paper for example, out of which he cut out some funny figures, small dolls in various stances. “These paper buffoons will now dance. Fetch me a few pins.” Soon each buffoon’s foot was pinned up. “This is for the buffoons not to be scattered and blown away by the newspaper,” Alex proclaimed arranging the figures on a tray, “The performance starts!” He “unglued” the newspaper from the stove and, holding it horizontally with both hands, brought it down to the tray with the figures. Alex commanded, “Stand up!” And just imagine: the figures obeyed. They stood up and stayed that way until he removed the newspaper when they lay down again. But he didn’t allow them to rest long: by alternately moving the newspaper to and from them he made the buffoons stand up and lie down again. “If I hadn’t burdened them with pins, they would have jumped up and stuck to the newspaper.” My brother took the pins out of some of the figures, “You see, they’ve stuck to the newspaper and won’t separate from it. This is electric attraction. And now we’ll experiment with electric repulsion, too. Where are the scissors?” I passed them to him and, having “glued” the newspaper to the stove, Alex began to cut a long, thin strip from its lower edge almost up to the upper one. Similarly, he made a second, third and other strip. When he got to about the sixth strip, he cut all the way to the edge. He had thus produced a sort of paper beard that didn’t slide down from the stove, as I had expected, but stayed put. Holding the upper part with one hand, Alex brushed along the strips several times 94-95 Figure 70 Figure 71 A Sheet of Newspaper and then took the “beard” down from the stove holding it at the top. Instead of freely dangling the strips spread out into a bell shape noticeably repelling one another. My brother explained, “They repel one another because they are charged up identically. However they are attracted to the things that are not charged. Poke your hand into the bell from below and the strips will be attracted to it.” I sat down and put my hand into the space between the strips. That is, I wanted to poke my hand there but couldn’t because the paper strips wound themselves round my hand like snakes. “Aren’t you frightened by these snakes?” asked Alex. “No, they are only paper.” “But I’m scared. Look, how scared.” Alex raised the newspaper above his head and I saw his long hair literally stand on end. “Is it another experiment?” “The same experiment we’ve just done, only another form of it. The newspaper electrified my hair and it is now attracted to the newspaper while each piece of hair repels the others like the strips of our paper beard. Look in the mirror and I’ll show you your own hair standing on end in the same fashion,” “Does it hurt?” “Not a bit.” Really, I felt not the slightest pain, not so much as tickling, although the mirror clearly showed to me that my hair under the newspaper stood on end. In addition, we repeated yesterday’s experiments and then my brother discontinued the “session”, as he called it, promising to do some new experiments tomorrow. A Sheet of Newspaper Miniature Lightning • Experiment with a Water Stream • Herculean Breath On the next night my brother Alex made some unu¬ sual preparations. He took three glasses, warmed them at the stove, put them on the table and covered with a tray that he had also preheated. “What is it going to be?” I inquired. “Shouldn’t the glasses be placed on the tray and not vice versa?” “Just wait, take your time. It’s going to be an experiment with miniature lightning.” Alex used the “electric machine” again-that is, he simply rubbed the newspaper on the stove. He then folded the newspaper in two and resumed the rubbing. Next he “unglued” it from the stove tiles and swiftly put on the tray. “Feel the tray... Is it cold?” Suspecting nothing, I light-heartedly stretched out my hand... and promptly jerked it back: something had cracked and pricked my finger painfully. Alex laughed, “How did you like it? You were struck by a lightning. Heard the crack? That was miniature thunder.” “I felt a strong prick, but I didn’t see any lightning.” “You will when we repeat it in the dark.” “But I won’t touch that tray any more,” I proclaimed decisively. “That’s not necessary, we can produce sparks, say, with a key or a tea-spoon. You’ll feel nothing, but the sparks will be as long as they were earlier. The first sparks I’ll extract myself while your eyes adapt to the dark.” He turned off the light. “Silence now. Keep your eyes open!” a voice said in the dark. Crack! and a bright bluish-white spark about 20 centimetres long darted between the edge of the tray and the key. “See the lightning? Hear the thunder?” “But they were at the same time. A real thunder always comes afteryou see the lightning.” “True. We always hear thunder later. Still, they occur simultaneously, rather like the crack and spark in our experiment.” “Why then is the thunder later?” “You see, lightning is light, and it travels so fast as to 96-97 A Sheet of Newspaper Figure 73 cover terrestrial distances in almost no time. Thunder is an explosion, i. e. sound, but sound travels in air not so fast and markedly lags behind the light, thus coming to us later. That’s why we see a lightning flash before we hear the accompanying thunder.” Alex passed me the key, removed the newspaper and-my eyes had now adapted-suggested extract a “lightning” from the tray. “Without the newspaper, will there be any spark?” “Just try.” I had hardly put the key near the tray edge when I saw a spark, long and bright. My brother again put the newspaper on the tray and again I extracted a spark, though it was weaker this time. He did so dozens of times (without rubbing the newspaper again on the stove), and each time I made a spark, which was getting ever weaker. “The sparks would continue for a longer time if I held the newspaper silk strings or ribbons rather than with my bare hands. When you study physics you’ll understand what occurred. Meanwhile it only remains for you to look with your eyes not head. Now one more experiment, with a water stream. We’ll make it in the kitchen at the water tap. Let the newspaper stay on the stove.” We make a thin stream of water from the tap so that it hits the basin bottom loudly. “Now, without touching the stream. I’ll make it fall somewhere else. Which way do you want it to be deflected, left, right, or forward?” I replied at random, “To the left.” “All right. Don’t touch the tap while I fetch the newspaper.” Alex was back with the newspaper, trying to hold it with his arms outstretched so as not to lose too much electricity. He brought the newspaper close to the stream from the left and I clearly saw it bend to the left. Having transferred the newspaper on the other side, he made the stream deflect to the right. Finally, he drew it forward so much that the water poured over the basin edge. “You see how strongly the attractive force of electricity manifests itself. By the way, this experiment can also be easily performed without a stove or oven. If, instead of the charged newspaper you take a conventional plastic comb like this one,” my brother produced a comb and passed it through his thick hair. 7-621 A Sheet of Newspaper “I have charged it up this way.” “But your hair is not electrical.” “No, it’s just like yours or anybody else’s. But if you rub plastic on your hair, it gets charged in the same way the newspaper does by the brush. Look.” When the comb was brought to the water stream, it made it deflect noticeably. “The comb is unsuitable for other our experiments since it accumulates too little electricity. It gets far less than the ‘electric machine’ that can be made from a simple newspaper. I’d like to make one more experiment with the newspaper, the last one. This time it’s not an electric experiment, but again one with air pressure, rather like the experiment with the ruler.” We returned to the sitting room and Alex began to cut and glue a long bag out of a newspaper. “While it dries, get several books, large and heavy.” On the bookshelf I found three massive volumes of some medical atlas and placed them on the table. My brother asked, “Can you inflate this bag with your mouth?” “Of course.” “A simple business, isn’t it? But what if I put a couple of these volumes on the bag?” “Oh, then the bag won’t inflate no matter how hard you try.” Alex silently put the bag at the edge of the table, covered it with one of the volumes and stood another one upright on it. “Just watch. I’ll inflate the bag.” “Perhaps you want to blow those books away?” I asked laughing. “Exactly.” Alex started to blow into the bag. Just imagine: as the bag swelled the lower book sloped up and overturned the top one. But the two books weighed about five kilograms! Without allowing me to recover from my surprise, Alex prepared to repeat the trick. This time he loaded the bag with all three tomes. He blew-a Herculian breath!-and the three tomes overturned. The amazing thing is that this experiment had nothing miraculous in it. When I dared to repeat it for myself, I managed to overturn the books as easily as Alex did. You need to have neither an elephant’s lungs nor the muscles of an athlet-everything comes about on its own accord, nearly without effort. 98-99 A Sheet of Newspaper My brother later explained the reason to me. When we inflated the paper bag, we forced some air into it that is more compressed than the air around us, otherwise the bag wouldn’t expand. The air outside presses down with about 1,000 grammes on each square centimetre. If you express the area under the books in square centimetres, you can readily work out that even if the excess pressure in the bag is only a tenth of that outside of it, i.e. a hundred grammes per square centimetre, then the total force from the air pressure inside the part of the bag under the books may be as high as 10 kilogrammes. Clearly this force is sufficient to overturn the books. Thus ended our physics tests with the newspaper. Seventy-Five More Questions and Experiments on Physics How to Weigh Accurately with An Inaccurate Balance Which is the more important possession, a precise pair of weighing scales or a precise set of weights? Many people believe that the scales are more important, but in fact-the weights, since it’s impossible to weigh anything accurately with inaccurate weights. If the set of weights is true, then you can still weigh quite accurately with inaccurate scales. For example, suppose you have beam scales with pans. Place a weight that is heavier than your object on one pan. Then on the other pan put as many weights as will be required to make the beam balance. Next put your object onto the pan with the weights and, of course, this pan will sink. In order to balance the beam again you will need to remove some of the weights and the weights removed will show the correct weight of your object. It should be clear why: your object now pulls down its pan with the same force with which the weights you took off did before. Hence your object and the total of the weights you took off weigh the same. This excellent way of weighing accurately using inaccurate scales was discovered by the great Russian chemist Dmitri Mendeleyev. On the Platform of a Weighing Machine A man stands on the platform of a weighing machine and suddenly he squats down. Which way will the platform move, up or down? The platform will move upwards. Why? Because as he is squatting the muscles pulling the man’s body down also pull the legs up, thus reducing the force with which the body presses on the platform with the result that it goes up. Weight on Pulley Suppose a man is able to lift a mass of 100 kilogrammes from the floor. Wanting to lift more he passed a rope tied tc the load through a pulley fixed in the ceiling (Fig. 76). What load will he be able to lift using this rig? Such a pulley could help him lift no more than what 100-101 Seventy-Five More Questions and Experiments on Physics he could do with his own hands, perhaps even less. If he pulled the rope passed through a fixed pulley, he could not lift a mass exceeding his own. If his mass is less than 100 kilogrammes, he would be unable to handle a 100-kilogramme load with the pulley. Two Harrows People often confuse weight and pressure. However, they are by no means the same. An object may have a marked weight but still exert a negligible pressure on its support. By contrast something else may have a small weight but exert a large pressure on its support. The following example will clarifythe difference between weight and pressure and at the same time give you an idea of how to work out the pressure a body exerts on its support. Let two harrows of the same type work in field, one with 20 teeth, the other with 60, the first one weighing 60 kilogrammes, the second 120 kilogrammes. Which one penetrates more deeply into the soil? It’s easy to figure out that the greater the force acting on a harrow’s teeth, the deeper they penetrate the soil. With the first harrow the total load of 60 kilogrammes is evenly distributed among the 20 teeth, hence 3 kilogrammes per tooth. With the second harrow, 120/60, i.e. 2 kilogrammes per tooth. Consequently, though in general the second harrow is heavier, its teeth penetrate less deeply than the first harrow’s. The pressure per tooth with the first harrow is larger than with the second. Pickled Cabbage Consider another simple calculation of the pressure. Two barrels of pickled cabbage are each covered with a wooden disk held down by stones. One disk is 24 centimetres across and the stones on it weigh 10 kilogrammes while the other is 32 centimetres across and its stones weigh 16 kilogrammes. In which is the pressure larger? Clearly, the pressure will be higher in the barrel where the load per square centimetre is larger. In the first case the 10 kilogrammes are distributed over an area’" of 3.14 x 12 x 12 = 452 square centimetres. * The area of a circle is about 3.14 times the circle’s radius (half the diameter) times the circle’s radius. Seventy-Five More Questions and Experiments on Physics Hence the pressure is 10,000/452, i.e. about 22 grammes per square centimetre. In the second barrel the pressure will be 16, 000/804, i.e. less than 20 grammes per square centimetre. The pickled cabbage is thus more compressed in the first barrel. Awl and Chisel Why does an awl penetrates deeper than a chisel does if both are acted upon by an equal force? The point is that when thrusting the awl all the force is concentrated at an extremely small area at its point. With the chisel the force is distributed over a much larger surface. For instance, let the awl’s surface area at the point be 1 square millimetre and the chisel’s be 1 square centimetre. If the force on each tool is one kilogramme, then the material under the chisel blade is subjected to a pressure of 1 kilogramme per square centimetre, and under the awl 1/0.01 = 100 or 100 kilogrammes per square centimetre (since 1 square millimetre = 0.01 square centimetre). The pressure of the awl is one hundred times larger than of the chisel. Now it is clear why the awl penetrates deeper than the chisel. You’ll now understand that when you are pressing with your finger on a needle when you are sewing you produce a very great pressure, not smaller than the steam pressure in a boiler. This is also the principle behind the cutting action of the razor. The slight force of hand creates a pressure of hundreds of kilogrammes per square centimetre on the thin edge of the razor that can cut through hair. Horse and Tractor A heavy crawler tractor is well supported by loose ground into which the legs of horses and people are mired. This is inconceivable to many people since the tractor is far heavier than the horse ana very much heavier than man. Why then do the horse’s legs are mired in loose ground, and the tractor doesn’t? To grasp this, you’ll have to remember once again the difference between weight and pressure. An object does not penetrate deeper because it is heavier but because it exerts a higher pressure (or force per square centimetre) on its support. The enormous weight of a crawler tractor is distributed over the larger 102-103 Seventy-Five More Questions and Experiments on Physics surface area of its tracks. Therefore, each square centimetre of the tractor’s support carries a load as low as several grammes. On the other hand, the horse’s weight is distributed over the small area under its hooves, thus giving more than 1,000 grammes per square centimetre or ten times more than the tractor. No wonder then that a horse’s feet sink more deeply into mud than does a heavy crawler tractor. Some of you may have seen that to ride over marshes and bogs horses are shod with wide “shoes”, which increase the supporting area of horses’ hooves with the result that they are mired much less. Crawling Over Ice If ice on a river or lake is insecure, experienced people crawl rather than walk over it. Why? When a man lies down, his weight, of course, doesn’t change, but the supporting area increases, each square centimetre of it thus carries less load. In other words, the man’s pressure on his support is reduced. It’s now clear why it’s safer to move over thin ice by crawling-this decreases the pressure on the ice. Some people also use a wide board and lie on it as they move about thin ice. What load can ice support without breaking? The answer is dependent on the thickness of the ice. Ice 4 cm thick can support a walking man. It is of interest to know the thickness of ice required for a skating rink on a river or lake. For this purpose 10-12 centimetres would be suflicient. Figure 77 Where Will the String Break? You’ll need an arrangement shown in Fig. 77. Put a stick on top of the open doors, tie a string to the stick and tie a heavy book in the middle. If now you pull a ruler tied to the bottom of the string, where will the string break: above or below the book? The string can break both above and below, according as you pull. It’s up to you, you can break it either way. If you pull carefully, the upper part of the string will break, but if you jerk it, the lower part breaks. Why does this happen? Careful pulling breaks the upper part of the string because the string is being pulled down both by the force of your hand and by the Seventy-Five More Questions and Experiments on Physics weight of the book, whilst the lower part of the string is only acted upon by the force of your hand. Whereas during the short instant of the jerk the book doesn’t acquire very much motion and therefore the upper part of the string doesn’t stretch. The entire force is thus “consumed” by the lower part, which breaks even if it’s thicker than the upper part. Torn Strip Figure 78 A strip of paper that is about 30 cm long and one centimetre wide can be material for a funny trick. Partly cut or tear the strip in two places (Fig. 78) and ask your friend what will happen to it if it’s pulled by the ends in the opposite directions. He will answer that it’ll break in the places where it’s been torn. “Into how many parts?” you ask then. Generally the answer is: “Into three parts, of course.” If you receive this answer, ask your friend to test his hunch by an experiment. Much to his surprise he will see that he was mistaken, for the strip will only separate into two parts. You can repeat the experiment many times taking strips of various length and making little tears of various depth and you’ll never get more than two pieces. The strip breaks where it’s weaker which goes to prove the proverb: “The chain is only as strong as its weakest link”. The reason is that of the two tears or cuts, however hard you strive to make them identical, one is bound to be deeper than the other. Even if it’s imperceptible to your eyes, one will still be deeper. The weakest place of the strip will be first to begin to break. And once begun the breaking would continue to the end because the strip would become ever weaker at this place. You might perhaps be very pleased to know that in making this trifling experiment you’ve visited a serious branch of science of importance for engineering that is called “strength of materials”. A Strong Match Box What will happen to an empty match box if you strike it with all your might? I’m sure that nine out of ten readers will sayring, I’ll try again.” “Why? Just cut the one you’ve got.” I did. This time I had two rings, no kidding. But when I wanted to separate them, it turned out that it was impossible to disentangle them for they were linked together. Brother was right, the ring was enchanted all right! “The trick is very simple,” my brother explained, “You can make such unusual rings for yourself. The key thing is that before you glue the ends of the paper strip twist one of them like this (Figure 3).” “Is it all because of that?” “Yes! Sure, I used an ordinary ring... It’ll be even more interesting, if the end is twisted twice, not just once.” Before my very eyes Alex prepared a ring in this way and handed it to me. “Cutting along the middle,” he said, “and see what happens.” I did and got two rings but one now went through the other. So funny, it was impossible to take them apart. I prepared three more rings for myself and obtained three more pairs of inseparable rings. “What would you do,” my brother asked again, “if you had to connect all four pairs of rings to form one long open-ended chain?” “Oh, this is simple: cut one ring in each pair, and glue them together again.” Alex enquired, “So, you would cut three of the rings?” By the Way “Of course.” “But what if you cut less than three?” “We have four pairs of rings, how can you possibly connect them by only breaking two rings? Impossible!” I was dead sure. In answer, my brother took the scissors, cut both rings in one pair and with them connected the remaining three pairs. Lo and behold! a chain of eight rings. Ridiculously simple! No trick in this and I could only be surprised why such a simple idea hadn’t occurred to me. “Enough of these paper rings. You’ve got some old postcards over there, it seems. Let’s have some fun with them, too. For instance, try and cut in a card the largest hole you can.” I punched the card with my scissors and carefully cut a rectangular hole in it, leaving only a narrow edge. “This is a hole among holes! A larger one is impossible!” I contentedly showed the result of my job to Alex. Of course, he had another opinion. “The hole is too small. Just enough for a hand to go through.” “You’d like it to be large enough for a head?” I retorted acidly. “The head and the body. So that you could thread all yourself through it. That would be some hole.” “Ha-ha! Do you really want to get a hole larger than the paper itself?” “Exactly. Many times larger.” “No trick will help you here. What is impossible is impossible...” “And what is possible is possible,” said Alex and set out to cut. Confident that he was joking, nevertheless, I watched him curiously. He bent the card in two, then drew two lines with a pencil near the long edges of the bent postcard and made two incisions near the other two edges. Next he cut the bent edge from point A to point 36-37 Figure 5 By the Way B and began to make a lot of cuts next to each other as shown in Figure 5. “Finished,” proclaimed my brother. “Why? I see no hole!” And Alex expanded the paper. Just imagine: it developed into a long-long chain that he easily threw over my head. It fell to my feet, zigzagging about me. “How can you get through such a hole? What do you say to that?” “Big enough for two!” I said with admiration. At that Alex finished his tricks, promising to treat me next time to a whole heap of new ones, this time only with coins. Tricks with Coins A visible and invisible coin* A bottomless glass* Where has the coin gone?* Arranging coins* Which hand holds the two-pence piece? * Shifting coins* An Indian legend* Problem solutions. “Yesterday you promised to show me a trick with coins,” I reminded my brother at breakfast. “Tricks? First thing in the morning? Hm, all right. Then empty the washing bowl.” Alex put a silver coin on the bottom of the empty bowl. “Look into the bowl without moving from your place and without leaning over. See the coin?” “Yes.” Alex pushed the bowl a bit farther away from me until I couldn’t see the coin any more since it was shielded by the side of the bowl. “Sit still, don’t move. I pour water into the bowl. What has happened to the coin?” “It’s visible again, as if it’s been lifted up together with the bottom. Why?” My brother sketched the bowl with the coin in it on a sheet of paper, and then everything became clear to Bay the Way Figure 6 1518 me. While the coin was at the bottom of the dry bowl, no ray of light could come from the coin because light travels in straight lines and the opaque sides of the bowl were just in the way. When the water was added, the situation changed since light rays coming from water into air get bent (physicists say “refracted”) and now can slid over the bowl edge and come into my eyes. However, we are used to seeing things only at a place where straight rays come from and this is why I mentally placed the coin somewhat higher than where it really was, that is along a continuation of the refracted ray. So it seemed to me that the bottom had risen with the coin. “I advise you to remember this experiment,” my brother added. “It will be useful when bathing. In a shallow place where you can see the bottom never forget that you see it higher than really is. And substantially so, for water appears to be shallower by about a quarter of its real depth. Where the actual depth is 1 metre, say, the apparent depth is only 75 centimetres. Bathing children often get into a trouble for this reason: relying on the deceptive appearance, they usually underestimate depth.” “I noticed that when you float slowly in a boat over a place where the bottom is visible, it appears that the greatest depth is just under the boat and it’s much shallower everywhere else. But shift to another place and again everywhere is shallow and beneath the boat is deep. It seems as if the deepest place travels with the boat. Why?” “Now you can understand that easily. The point is that the rays coming straight up out of the water change direction least of all, thus the bottom there appears to be less elevated than the places which send oblique rays to our eyes. Naturally, the deepest place appears to us to lie just beneath the boat even if the bottom were perfectly flat. But now let’s do quite another experiment.” Alex filled a glass with water right up to the brim. “What do you think will happen if now I drop a two-pence piece into the glass?” “The water will overflow, of course.” “Let’s try.” Carefully, without jerking, my brother lowered the coin into the brimful glass. Not a drop overflowed. “Now let’s put in another coin,” he said. I warned him, “Now it’s sure to overflow.” 38-39 By the Way And I was mistaken: in the full glass there was room for the second coin, too. A third and a fourth coin followed each other into the glass. “What a bottomless glass!” I exclaimed. Alex silently and cooly kept on lowering one coin after another into the glass. A fifth, sixth, seventh time coins fell onto the bottom-no overflowing. I couldn’t believe my eyes and was impatient to find out the explanation. But my brother took his time to explain, he was still carefully dropping coins and only stopped at the 15th two-pence piece. “Well, that’ll do,” he said at last, “Take a look, the water has bulged up at the glass’s edge.” Indeed, the water had bulged above the edge by about the thickness of a match, sloping down at the edges as if it were in a transparent bag. Alex went on to say, “The answer lies in the bulging. This is where the water is that was expelled by the coins.” “Fifteen coins have displaced so little water?” I was astounded. The stack of 15 two-pence pieces is rather high but here is only a thin layer, just thicker than a penny.” “Take its area into consideration, not only the thickness. The layer may be not thicker thanthat the box won’t survive such handling. The tenth-the person 104-105 Seventy-Five More Questions and Experiments on Physics Figure 79 Figure 80 who has actually performed the experiment or heard about it from somebody - will maintain that the box will survive. The experiment should be staged as follows. Put the parts of an empty box one on top of the other, as shown in Fig. 79. Strike this assembly sharply with your fist. What will occur will surprise you: both parts will fly apart but, having collected them, you’ll find that each one is intact. The box behaves like a spring and this saves it because it bends but doesn’t break. Bringing Something Closer by Blowing Place an empty match on a table and ask somebody to move it away by blowing. Clearly this is no problem. Then ask him or her to do the opposite, i.e. make the box approach without leaning forward to blow the box from behind. There’ll hardly be many who’ll twig. Some will try to move the box nearer by sucking in air, but that won’t work of course. The answer, however, is very simple. What is it? Ask somebody to put the hand vertically behind the box. Begin to blow and the air that reflects from the hand will strike the box and shift it towards you (Fig. 80). The experiment is, so to speak, “failsafe”. You’ll only have to make sure it’s on a sufficiently smooth table (even unpolished) which is not of course covered with a table-cloth. Grandfather's Clock Suppose a grandfather’s clock that uses weights to wind it up is fast or slow. What should be done with the pendulum to correct it? The shorter a pendulum the quicker it swings. You Seventy-Five More Questions and Experiments on Physics can easily prove this by an experiment with a weight suspended from a piece of rope. This suggests the solution of our problem: when the clock is slow you shorten the pendulum a little by lifting a ring on the pendulum rod, so making the pendulum swing faster; and when the clock is fast you lengthen the pendulum. Figure 81 How Will Rod Settle Down? Two balls of equal mass are fixed to the ends of a rod (Fig. 81). Right in the middle of the rod a hole is drilled through which a spoke is passed. If the rod is spun about the spoke, it’ll rotate several times and settle down. Could you predict in what position the rod will come to rest? Those who think that the rod will invariably settle down in a horizontal position are mistaken. It can remain balanced in any position (see Fig. 81)-horizontal, vertical, or at an angle-since it’s supported at the centre of mass. Any body supported or suspended at the centre of mass be in equilibrium at any position. Therefore, it’s impossible to predict the final position of the rod. Jumping in Railway Carriage Imagine you are travelling in a train at a speed of 36 kilometres an hour and you jump up. Supposing that you manage to spend a whole second in the air (a brave assumption because you’ll need to jump up more than a metre), where will you land, at the same place from where you started or somewhere else? If somewhere else, where then-closer to the beginning or end of the train? You’ll land at the same place. You shouldn’t think that while you’ve been in the air the floor (together with the carriage) has shifted forward. To be sure, the carriage was tearing along but you also were travelling in the same direction and at the same speed carried by inertia. All the time you were directly above the place from which you jumped up. Aboard a Ship Two people are playing ball on the deck of a steaming vessel (Fig. 82). One stands nearer the aft and the other 106-107 Figure 82 Seventy-Five More Questions and Experiments on Physics nearer the bows. Which one can throw the ball easier to his partner? If the ship is travelling with a steady speed and in a straight line neither has any advantage, just as if they were on a stationary ship. You should not suppose that the man standing nearer the bows recedes from the ball after it’s been thrown or that the other man moves to meet it. By inertia the ball has the ship’s speed which is equally possessed by both partners and the ball. There¬ fore, the motion of the ship (uniform and rectilinear) gives neither player an advantage. Flags A balloon is being carried away due north. In which direction will flags on its car fly? The balloon carried by an air flow is at rest with respect to the surrounding air, therefore the flags won’t be blown by the wind, but will dangle limply like they do in still weather. On a Balloon A balloon floats motionlessly in the air. A man gets out of the car and begins to climb up the cable. Which way will the balloon move in the process, upwards or downwards? The balloon will shift downwards, since the man pushes the cable (and the balloon) in the opposite di¬ rection as he is climbing. The situation is similar to what happens if someone walks forward over the bottom of a small rowing boat: the boat shifts backwards. Walking and Running What is the difference between running and walking? Before answering remember that running can be Figure 83 Seventy-Five More Questions and Experiments on Physics slower than walking and that you can even run on the spot. The difference between running and walking is not the speed. When we walk our body is in contact with the ground all the time at some point in our feet. When we run, on the other hand, there are moments when the body is completely separated from the ground and does not touch it at any point. A Self-Balancing Stick Put a smooth stick on the index fingers of both of your hands, as shown in Fig. 83. Now move your fingers together to meet each other half-way. Strangely, in the final position the stick doesn’t fall off but keeps its balance. Make the experiment several times varying the initial position of your fingers, the result will invariably be the same: the stick will be balanced each time. Replace the stick by a ruler, a billiards cue, or a broom, and you’ll notice the same behaviour. What is the secret? The following is clear: if the stick is balanced on your fingers brought together, this suggests that your fingers have closed up under the centre of mass (a body is in equilibrium if the centre of mass is over an area confined by the support’s boundaries). When your fingers are spread apart, the larger load is on the finger that is closer to the stick’s centre of mass. Friction increases as the load grows and the finger closer to the centre of mass is subject to larger friction than the other one. Therefore, the finger that is closer to the centre of mass doesn’t slide under the stick and at all times the only finger that moves is the one farther away from this point. Once the moving finger is closer to the centre of mass than the other, the fingers change their roles, the change taking place several times until the fingers come together. Since only one finger is moving at each instant of time, namely the one that is 108-109 Seventy-Five More Questions and Experiments on Physics farther away from the centre of mass, it’s only natural that eventually both fingers end up under the centre of mass of the stick. Before we leave this experiment, we’ll repeat it with a broom (the top of Fig. 84) and ask ourselves what would happen if we cut the broom at where it’s supported by the fingers and place the parts on different pans, which pan would sink? Figure 84 It would seem that if both parts of the broom balance each other on your fingers these should also do so on the pans of the scales. Actually, the part with the brush will outweigh. The clue is not difficult to find, if we take into account that when the broom was balanced on your fingers the gravity forces of both parts were applied to unequal arms of the lever. On the pans of the scales, by contrast, the same forces are appliedto the ends of an equal-arm lever. Rowing in the River A rowing boat and wooden chip alongside it are floating in a river. What is it easier for the rower: to get ahead of the chip by 10 metres or to lag behind it by 10 metres? Even those practising water sports often give the wrong answer. It’s more difficult, they argue, to row upstream than downstream, accordingly, to pass the chip is easier than to lag behind it. No doubt, to reach a point rowing upstream is more difficult than rowing downstream. But if the point you are going to reach is floating alongside, just like our chip, the situation is quite different. One should take into account that the boat carried by the current is at rest with respect to the water. The situation is the same as what it would be on the still water of a lake. Thus, in both cases the rower needs exactly the same effort whether he wishes to pass or lag behind the boat. Seventy-Five More Questions and Experiments on Physics Circles on Water A stone thrown into still water produces concentric waves. What form will the waves have if the stone is thrown into the flowing water of a river? If you fail, from the very beginning, to follow the right track, you’ll be easily lost in the argument and come to the conclusion that in the flowing water the waves should assume the form of an ellipse or an oblong somewhat wider in the upstream direction. But if we attentively observe the waves produced by a stone thrown into the river, we’ll find no deviation from the circular shape, however fast the stream is. There is nothing extraordinary in that. Simple reasoning will lead to the conclusion that the waves should be circular both in still and in flowing water. Let’s treat the motion of particles of the waves as a combination of two movements: radial (from the centre of oscillations) and translational (downstream). A body participating in several motions eventually comes to the same point it would come to, if it performed all the component motions in succession. We’ll therefore assume that the stone is thrown into still water. In that case, the waves will clearly be circular. Now suppose that the water is moving-no matter with what velocity, uniformly or not-the motion has only to be translational. What will happen to the circular waves? They’ll undergo a translation without any distortion, i.e. will remain circular. Deflection of Candle Flame If you carry a candle about a room you will have noticed that initially the flame deflects backwards. Which way will it deflect if the candle is carried about in a closed casing? Which way will the flame in the casing deflect if it’s uniformly rotated, horizontally in an outstretched hand? If you think that in the casing there’ll be no deflection, you are mistaken. Experiment with a burning match and you’ll see that if it’s protected by the hand as it’s moved, the flame will deflect, but forwards-quite unexpectedly!-not backwards. This is because the flame is thinner than the surrounding air. A force imparts to a body with a small mass a larger velocity than to a body with a larger mass. Therefore. 110-111 Seventy-Five More Questions and Experiments on Physics the flame moving faster than the air in the casing deflects forwards. The same reason (the smaller density of the flame than that of the surrounding air) also accounts for the unexpected behaviour of the flame when we move the casing in a circle, the flame deflects inwards, not outwards as might be expected. This would be clear if we remember how mercury and water are arranged in a ball rotated in a centrifuge. The mercury tries to be farther away from the rotation axis than the water. The latter, as it were, floats up in the mercury, if we consider the “bottom” to be the direction away from the rotational axis (i.e. the one in which bodies are displaced by the centrifugal effect). In our circular rotation, the lighter-than-air flame “floats up” within the casing, i.e. in the direction to the rotation axis. A Sagging Rope With what force must one pull at a rope for the latter not to sag? However taut the rope is, it is bound to sag. Gravity that causes the sagging acts normally, whereas the stretching force on the rope has no vertical component. Two such forces can never balance each other out, i.e. their resultant force cannot be zero. And this resultant force is responsible for the sagging. No force, however strong, can stretch a rope strictly horizontally (except when the rope is upright). The sagging is unavoidable, you can reduce it to a desired degree but cannot make it zero. Consequently, any nonvertically stretched rope or driving belt will sag. For the same reason it is impossible, by the way, to stretch a hammock so that its ropes are horizontal. The taut net of a bed sags under the weight of a man. And the hammock, whose ropes are not so taut, turns into a dangling bag when a man lies on it. How to Drop a Bottle? In which direction with respect to a moving railway carriage should you throw a bottle so that the danger that it gets broken when hitting the ground is the least? As it is safer to jump forwards from a moving carriage, it would appear that the bottle would not hit the ground so strongly if you throw it forwards. This is not so: objects should be thrown backwards. In that Seventy-Five More Questions and Experiments on Physics case the velocity imparted to the bottle by throwing it will be subtracted from the one due to inertia with the result that the bottle will strike the ground with a smaller velocity. Throwing the bottle forwards will cause the reverse, the velocities would add up and the collision would be stronger. That it is safer for a man to jump forward is accounted for by quite a different reason: he is hurt less by jumping this way. Cork A piece of cork has got into a bottle with water. The cork is small enough to pass freely through the neck, but try as you can, shaking or upending the bottle, the outpouring water will not for some reason bring the cork out. It’s only when the bottle is completely empty that the cork leaves the bottle with the last bit of the water. Why? The water doesn’t bring the cork out for the simple reason that cork is lighter than water and therefore is always on its surface. The cork can only come to the opening when almost all of the water has come out. That’s why it is the last to leave the bottle. Floods During a spring flood the surface of a river becomes convex-higher in the middle than near the banks. If loose logs float along such a swollen river, they will slide down to the banks leaving the mainstream free (the top of Fig. 85). In midsummer, when the water is low, the river surface becomes concave - lower in the middle than near the banks. In this case logs will accu¬ mulate in the middle (the bottom of Fig. 85). What’s the reason? This is explained by the fact that in the middle water flows quicker than near the banks because the friction Figure 85 112-113 Seventy-Five More Questions and Experiments on Physics of the water along the bank slows the current down. During a flood, water comes from the upper reaches faster along the middle than near the banks because the current’s speed is faster in the middle. Understandably, if more water comes to the middle, then the river should swell here. The situation changes in midsummer when water subsides. Now, owing to the swifter current the water run-off in the middle is higher than near the banks with the result that the river becomes concave. Liquids... Press Upwards! That liquids exert a pressure downwards, on the bottom of a vessel, and sidewards, on its walls, is known even to those who have never studied physics. But many people don’t suspect that liquids press upwards as well. A glass tube will help you to make sure such a pressure does exist. Cut out a diskof a strong cardboard, its size being sufficient to cover the hole of the tube. Put it over the hole and dip both into some water. For the disk not to drop off when you are dipping it, it can be held by a piece of string passed through its centre or pressed on with a finger. When the tube has sunk to a certain depth, you will notice that the disk holds securely on its own without being pressed on with the finger or held with the string, being supported by the water that presses it up. You can even measure the amount of this upward pressure. Carefully pour some water into the tube. Once the water level approaches the level outside the tube, the disk will fall off. The water pressure on the disk from below is thus balanced out by the pressure of the water column within the tube, its height being equal to the depth of the disk in the water. This is a law about the pressure of liquids on a submerged body. By the way, this also causes the weight “loss” in liquids and was formulated as the famous Archimedes principle. Figure 86 8-621 Seventy-Five More Questions and Experiments on Physics If you have several glass tubes of various shapes but with the same opening (e. g. as shown in Fig. 86) you can also test another law relating to liquids, namely the pressure of a liquid on the bottom of a vessel is only dependent on the bottom area and the level and is independent of the vessel shape. An experiment with the various glass tubes is described below. Dip them into the water to the same depth (for which purpose you’ll have to glue paper strips onto them at the same height) and you’ll notice that the disk will always fall off at the same level of the water within the tube (Fig. 86). In consequence, the pressure due to water columns of various shapes is the same if only their base areas and heights are the same. Notice that it’s the height, not the length, that matters because a long inclined column exerts exactly the same pressure on the bottom as a short upright column of the same height (the base areas being equal). Which is Heavier? On one pan of scales is placed a pail that is filled to the brim with water. On the other pan, exactly the same sized pail is placed, also brimful, but with a piece of wood floating in it (Fig. 87). Which pail will be heavier? Figure 87 I asked various people this question and got conflicting answers. Some answered that the pail with the wood would be heavier because “the pail has the water and the wood.” Others held that, on the contrary, the first pail would be heavier “since water is heavier than wood.” Both views are a mistake for both pails have the same weight. True, there is less water in the second pail than in the first because the floating piece of wood displaces some water. The immersed part of every floating body displaces exactly the same weight of water as the whole of the body weighs. That’s why the scales will be in equilibrium. Another problem. Suppose I place on the scales 114-115 Seventy-Five More Questions and Experiments on Physics Figure 88 a glass of water and put a weight near it. When the system is balanced by the weights on the other pan, I drop a weight into the glass. What will happen with the balance? According to the Archimedes principle the weight in the water becomes lighter than before. It might be expected that the pan with the glass would rise but in actual fact the scales will remain in equilibrium. Explain. The weight in the glass has displaced some water, which has risen above the initial level, with the result that the pressure on the bottom of the vessel has increased so that the bottom is acted upon by an added force equal to the weight lost by the weight. Water on a Screen It turns out that water can be carried on a screen in real life and not only in fairy tales. A knowledge of physics will help to make this proverbially impossible thing possible. You’ll need a wire screen about 15 centimetres across with a mesh size of about 1 millimetre. Immerse the network into melted wax and when it is taken out of the wax the wire will be covered with a thin layer of wax hardly noticeable for the naked eye. The screen will still remain a screen - a pin will freely pass through its mesh-but now you will be able literally to carry water on it. The screen will hold a fairly high level of water without any seepage through the mesh. You need only to pour the water carefully and see to it that the screen is not jerked. Why then doesn’t the water seep? Because it doesn’t wet wax and thus forms thin films between the meshes and it is the films’ downward convexity that holds the water (Fig. 88). Such a waxed screen may be placed on water and it will remain on the surface. It is thus possible not only to carry water on a screen but to float on it too. This paradoxical experiment accounts for a number of the everyday phenomena we take for granted because we get used to them so. Tarring barrels and boats, painting with oil paints and, in general, coating things we want to render water-tight with oily materials, and the rubberizing of fabrics, these are all nothing but the making of “screens” like the one just described. The idea behind each phenomenon is the Seventy-Five More Questions and Experiments on Physics same. Only in the case of the screen it appears in a somewhat unusual disguise. Soap Bubbles Can you make soap bubbles? This is not as simple as it might seem. I also once thought that it didn’t take much dexterity until I found out practically that blowing large and beautiful bubbles is an art that requires much exercise. But is it worthwhile to occupy yourself with such a trifling business as blowing soap bubbles? Used as a figure of speech the notion of soap bubbles is not complimentary. But the physicist has another view of them. The great English scientist Lord Kelvin wrote, “Blow a soap bubble and observe it, it may take a lifetime to investigate it, incessantly deriving lessons of physics from it.” Indeed, the fabulous play of colours on the surface of thin soap films enables physicists to measure the wavelengths of light, and the study of the tension in these frail films gives an insight into the laws governing the interaction between particles, those cohesion forces without which there would be nothing in the world but fine dust. The several experiments that follow do not pursue such serious objectives, they are just amusements that will only acquaint you with the art of blowing soap bubbles. In his book Soap Bubbles the English physicist Charles Boys gave a detailed account of a number of experiments involving them. Those interested are referred to this fascinating book, but we’ll only describe the simplest of the experiments here. These can be performed using a solution of a conventional soap*, but for best results olive- or almond-oil soaps are recommended. A piece of soap is carefully dissolved in pure cold water until a fairly thick solution is obtained. Rain or thaw water is the best but if it’s unavailable cooled boiled water will do. For bubbles to have a long life it is recommended to add one third of the volume of glycerin. Using a spoon, remove foam and bubbles from the surface and insert into it a long clay tube whose end on the outside and inside has already been smeared with soap. Good results are also achieved with straws about 10 Toilet soaps are unsuitable. 116-117 Seventy-Five More Questions and Experiments on Physics Figure 89 centimetres long that are split across the end. The bubbles are blown thus: dip the tube into the solution holding it upright so that a liquid film be formed at the end and carefully blow into it. Since the bubble is filled with warm air from your lungs, which is lighter than the surrounding air in the room, the bubble just blown will rise into the air. If from the very beginning you can producea bubble 10 centimetres in diameter, the solution is good, otherwise some more soap will have to be added to the liquid until bubbles of the above-mentioned size are obtained. But this test is not sufficient. When a bubble is produced, dip a finger into the soap solution and try to punch the bubble. If it doesn’t burst you may proceed to the experiments, but if the bubble doesn’t survive the test, add some more soap. Experiments should be carried out carefully, slowly, and quietly. If possible, the illumination should be bright, otherwise the bubbles will not show their iridescent play. The following are a number of entertaining experiments with soap bubbles. A Bubble Around a Flower. Pour some soap solution onto a plate or a tray so that the bottom is covered with a layer 2-3 mm thick. Place a flower or small vase in the middle and cover it with a glass funnel. Then, slowly lifting the funnel, blow into the narrow tube to form a soap bubble. Once the bubble has reached a largish size, tip the funnel over as shown in Fig. 89, and liberate the bubble from under it. The flower will then be under a transparent hemispherical hood of soap film which will show all the colours of the rainbow. Instead of a flower you can take a small statue and crown its head with a soap bubble. First you need to drop some solution onto the head of the statue and then, after blowing the large bubble, pierce it and blow a smaller one inside it. Bubbles Inside One Another. Blow a large bubble using the funnel, then immerse a straw into the soap solution so that only the end you will put into your mouth is dry and poke it carefully through the wall of the first bubble to the centre. By carefully drawing the straw back, a second bubble can be blown inside the first one, then a third, fourth, and so on. A Cylinder of Soap Film (Fig. 90) can be blown between two wire rings. In order to do this lower Seventy-Five More Questions and Experiments on Physics a conventional ball-shaped bubble onto the bottom ring. Then put a wetted second ring over the top of the bubble and by raising it the bubble will extend until it becomes cylindrical. Curiously enough, if you raise the upper ring higher than the length of the ring’s circum¬ ference, the cylinder will become narrower at one end and wider at the other, and then it will disintegrate into two bubbles. The film of a soap bubble is always in tension and exerts a pressure on the air inside it. By directing the funnel at the flame of a candle you can make sure that the force of the thin film is not all that negligible since the flame will be deflected quite a bit (Fig. 90). It is interesting just to observe a bubble when it is taken from a warm room into a cold one. It will shrink appreciably, and conversely it will expand when brought from the cold room into the warm one. Clearly, the reason is that the air in the bubble expands and contracts. If, for example, the volume of a bubble at — 15 °C is 1,000 cubic centimetres and the bubble is brought into a room at -I- 15 °C, its volume will increase by about 1,000x 30x 1/273 or about 110 cubic centimetres. Furthermore, it should be noted that the common idea that soap bubbles are short-lived is wrong since with adequate handling a soap bubble can survive for weeks. The English physicist Dewar (famous for his works on air liquefaction) kept soap bubbles in special bottles that were protected from dust, drying and jerks. Under these conditions he managed to keep some bubbles for a month or so. An American, Lawrence, succeeded in keeping soap bubbles in a glass cup for years. An Improved Funnel Those who have poured water through a funnel into a bottle know that it is necessary to raise the funnel from time to time, otherwise the liquid will not pour out of it. It’s the air inside the bottle that, when compressed by the incoming liquid and unable to escape, stops more liquid from coming in from the funnel. Understandably, by raising the funnel we let the compressed air out, thus again enabling some more liquid to go in. It would perhaps be quite practical to design a funnel so that it has longitudinal crests on its outer surface 118-119 Seventy-Five More Questions and Experiments on Physics that would keep the funnel from sticking to the bottleneck. But I haven’t ever seen such a funnel in everyday life, only in laboratories they use a filter designed after this fashion. How Much Does Water Weigh in a Glass Held Upside-Down? Figure 91 You’d say, “Nothing, of course. Water won’t stay in the glass.” I’d ask, ’’And if it does stay, what then?” Actually, it is possible to keep water in a glass held upside-down so that it doesn’t pour out. The method is shown in Fig. 91. An upturned goblet tied at the bottom on one side of a balance is filled with water so that it doesn’t pour out because the goblet’s edges are immersed in water. On the other side of the balance tie an empty goblet, exactly the same sort. Which side will go down? That to which the upturned goblet with water is tied. This goblet is exposed to atmospheric pressure from above, and from below-to the atmospheric pressure minus the weight of the water contained in the goblet. For the system to be in balance you’d have to fill the other goblet with water. Accordingly, the water in the upturned glass weighs in these circumstances as much as it would in a normally held glass. How Much Does the Air in a Room Weigh? Can you say, however inaccurately, how much the air in a small room weighs? Several grammes or several kilogrammes? Would you be able to lift such a load with a finger or would it be difficult to hold it on your back. Perhaps these days there is no one who believes air is weightless as was widely held in ancient times. But even today many wouldn’t estimate its weight. Remember that a litre jar of the warm summer air near the ground (not in the mountains) weighs 1.2 grammes. A cubic metre holds 1,000 litres and therefore weighs 1,000 times as much, i.e. 1.2 kilogrammes. Now we can easily work out the weight of the air in a room. To do so, we’ll only need to know how many cubic metres there are in it. If, say, the area of the room is 15 square metres, the height is 3 metres, then it Seventy-Five More Questions and Experiments on Physics contains 15 x 3 = 45 cubic metres. The air thus weighs 45 kilogrammes plus 1/5 of 45, i.e. 9 kilogrammes, which makes 54 kilogrammes in all. You could not move this load with a finger or carry it about on your back with ease. An Unruly Cork This experiment will vividly demonstrate that compressed air has a force and an appreciable one at that. For the experiment we’ll only need a common bottle and a cork that’s somewhat smaller than the bottleneck. Hold the bottle horizontally, insert the cork into the neck and ask somebody to blow the cork inside the bottle. No problem, it would seem. But try it, blow hard at the cork, you’ll be amazed at the result. The cork won’t be driven inside the bottle but... will fly into your face! The harder you blow the faster it’ll shoot out. If you want the cork to slide inside you’ll have to do quite the opposite-not to blow at the cork but to suck the air from the hole. These strange phenomena can be explained as follows. When you blow into the bottleneck you drive some air through the gap betwen the cork and the wall of the neck. This increases the pressure inside the bottle and throws the cork out. If then you suck the air out, the air inside the bottle becomes thinner and the cork is pushed inside by the pressure of the air outside. The trick works out well only when the neck is absolutely dry as a wet cork sticks. The Fate of a Balloon Balloons sometimes go astray. But where? How high can they fly? A balloon that escapes is carried always not to the boundaries of the atmosphere, but only to its “ceiling”,i.e. to a height where the air is thin and the weight of the balloon equals that of the air displaced by it. But it does not always reach its ceiling. Since it swells (due to the reduction in the external pressure) it may burst before it reaches the ceiling. 120-121 Seventy-Five More Questions and Experiments on Physics How to Blow Out a Candle? It’s child’s play, you might think, to blow out a candle. But occasionally an attempt is a failure. Try and blow a candle out through a funnel and you’ll see that this requires especial dexterity. Place the funnel against the flame of a candle and blow at it through the thin end. The flame won’t so much as stir, although the stream of air from the funnel would seem to be striking the flame directly. Perhaps you now think the funnel is too far away from the flame, and so you bring it nearer and again begin to blow hard. You might be shocked by the result: the flame deflects not away from you but towards you, against the stream of the air coming from the funnel. What is to be done then to kill the candle flame? It is necessary to locate the funnel so that the flame is not on the axis of the funnel but in the line of its cone part. Now by blowing into the funnel you’ll easily extinguish the candle. This is explained by the fact that the air stream leaving the narrow part of the funnel does not propagate along its axis but spreads along the walls of the cone, thus forming a sort of an air vortex. But the air along the funnel axis is rarefied with the result that a return air flow sets in near it. It is now clear why a flame located on the axis of the funnel leans towards the funnel, and when the flame is on the periphery of the cone, it bends the other way and goes out. Tyre A car wheel with a tyre is rolling to the right, its rim rotating clockwise. The question is: in what direction does the air inside the tyre move-against the direction of rotation or in the same direction? The air moves away from the place of compression in both directions - forwards and backwards. Why Are There Gaps Between the Rails? Railway builders always leave gaps between the butts of adjacent rails on purpose. Without the gaps the railway would soon fall into disrepair. The reason is that all things expand on heating. A steel rail, too, elongates in summer, heated by the sun. If no space were allowed for the rails to expand, these would push against Figure 92 Seventy-Five More Questions and Experiments on Physics adjacent rails with an enormous force and bend sideways wrenching out the spikes and destroying the track. The gaps are designed with due account of winter temperatures. In winter the rails shrink from cold, thereby additionally increasing the gaps. Therefore, they are calculated very carefully considering the local climate. An example of the use of the property of a body to shrink on cooling is the old procedure of shoeing cart wheels. A heated iron shoe is slided onto the rim of a cart wheel. When the shoe is allowed to cool down, it shrinks and squeezes tightly onto the rim. A Glass and Tumbler You may have noticed that tumblers for cold drinks are often made with a thick bottom. The reason is obvious: such a tumbler is more stable. Why then don’t we use tumblers for hot drinks? After all it would be better for glasses to be more stable in that case too. Thick-bottomed tumblers are not used for hot drinks because the walls of such tumblers would be heated by the hot liquid and expand more than the thick bottom. The thinner the glassware and the less difference there is between the thickness of the wall and the bottom, the more uniform will be the heating and the less the risk of cracking. The Hole in the Cap of a Tea-Kettle The cap of a metallic tea-kettle has a hole. What for? To let some vapour out, otherwise it will pop the cap off. But the cap expands on heating in all directions. What happens to the hole in the process? Does it become narrower or wider? It becomes wider. In general the volume of holes and cavities becomes larger on heating in exactly the same way as an equal piece of surrounding material does. For that reason, by the way, the capacity of vessels increases on heating, not decreases as is widely believed. Smoke Why does smoke go up in still weather? TTie smoke from a chimney ascends because it’s 122-123 Seventy-Five More Questions and Experiments on Physics carried by hot air that expands on heating, thus becoming lighter than the air around the chimney. When the air supporting the smoke particles cools down, the smoke descends and spreads out over the ground. Incombustible Paper We can perform an experiment in which a paper strip doesn’t bum in the flame of a candle. Wind a narrow paper strip tightly around an iron rod. If now you introduce the rod with the wound strip into the flame of a candle, the paper won’t catch fire. The fire will lick the paper, the latter will char but not bum down until the rod becomes hot. Why? Because iron, just like any metal, is a good heat conductor; it leads away the heat obtained by the paper from the flames. Replace the metal rod by a wooden stick and the paper will bum because wood is a poor heat conductor. With a copper rod the experiment is even more successful. Instead of the paper strip you could also use a piece of string wound tightly around a key. How to Seal Window Frames for Winter An adequately sealed window frame keeps out cold. But to seal it properly you should get it right why the frame “heats” a room. Many believe that a second frame is used in winter because two windows are better than one. That is not so. It’s not the second window that matters here but the air confined between the windows. Air is a very poor heat conductor. Therefore, some air adequately confined for it not to carry any heat away prevents the room from cooling. But for best results the air must be sealed tightly inside. Some people wrongly think that when a frame is sealed for the winter the upper gap in the external frame should be left unsealed. Should you do so the air within the cavity would be displaced by outside cold air, thus chilling the room. On the contrary, both frames should be treated painstakingly and not even the tiniest chink should be left. Alternatively, you can with good results glue frames over with strips of strong paper. Well sealed or glued windows cut down your heating expenses. Seventy-Five More Questions and Experiments on Physics Draught from a Closed Window It might seem unusual that in a cold weather there is often a draught from a window that is tightly closed, carefully sealed and does not have the smallest hole. There is nothing surprising about that. The air inside a room is almost never at rest. There are invisible flows caused by the heating and cooling of the air. Heating makes air thinner, and hence lighter. Conversely, cooling makes it denser and heavier. The light, heated air over a lamp or stove is displaced by cold air up to the ceiling because the heavy air that has cooled near the windows or cold walls, flows down to the floor. These currents in a room are readily discovered using a balloon with a small weight attached to it for it not to strike the ceiling and float freely in the air. Let the balloon go near a warm stove and it’ll travel about the room pulled around by the invisible air currents: from the stove to the window under the ceiling, then down to the floor and back to the stove for a new cycle. That’s why in winter we feel a draught from a window, especially at the bottom, even though the frame is securely sealed and keeps the outside air out. How to Chill with Ice If you want to chill a bottle of drink, where should you place it, on or under the ice? Many put a bottle on the ice without a moment’s hesitation, just like they put a tea kettle on a fire.That’s not the way to do it. Heating should be done from below, but chilling, on the contrary, is better from the top. Explain why. You know that colder substances are denser than warm ones. Thus a chilled beverage is denser than a warm one. When you place the ice over the top of the bottle, the upper portions of the drink (adjacent to the ice) sink on cooling being replaced by another amount of the liquid that in turn cools down and descends as well. In a short while all the drink in the bottle will have been in contact with the ice and chilled. But if the bottle is placed over the ice, the lowest portion cools first, its density increases and it stays at the bottom making no room for the rest of the liquid that is warmer. No mixing occurs here and the chilling is extremely poor. 124-125 Seventy-Five More Questions and Experiments on Physics It pays to chill everything from the top and not just drinks-meat, vegetables and fish should be placed under ice as well. They are chilled not so much by the ice itself as by the surrounding air because the cold air comes down. If you need to cool a room with ice don’t place it on the floor but put it up high on a shelf or suspend from the ceiling. The Colour of Water Vapour Have you ever seen water vapour? Could you say what colour it is? Strictly speaking, water vapour is absolutely transparent and colourless. It is invisible, just like air. The white fog that is popularly known as “vapour” is really a multitude of water droplets, it is a suspension of fine water particles, not vapour. Why Does a Boiler “Sing"? A boiler or a kettle produces a singing sound when the water is about to boil. The water adjacent to the heater vaporizes to form small bubbles. Being much lighter these are expelled upwards by the surrounding water and as they go up the bubbles pass through water that has a temperature of less than 100 °C. The vapour in the bubbles cools, contracts and the bubbles collapse under pressure. Thus, just before boiling sets in, more and more bubbles go up but fail to reach the surface collapsing on the way to produce a cracking sound. It is these numerous cracking that produce the sound we hear at the outset of boiling. When the water eventually heats to boiling temperature, the bubbles cease to collapse on their way up and the “singing” discontinues. However, once the water starts to cool down, again the earlier conditions occur and the “singing” resumes. A Miraculous Top Cut a small square out of thin tissue-paper. Fold it diagonally twice and smooth it out again. You’ll thus know where the centre of mass of the square is. Now place the paper on the point of an upright needle so that the latter supports it at the middle. The paper will balance since it’s supported at the centre of mass. A slightest flow of air will make it Seventy-Five More Questions and Experiments on Physics rotate on the needle. So far there is nothing miraculous about it. But bring your hand close to the paper as shown in Fig. 93. Do it carefully so that the paper is not swept away by the air flow. A strange thing will happen, the paper will start rotating, slowly at first but then faster. Remove your hand and the rotation will stop. Bring it close again and it will start again. This miraculous rotation at one time-in the 1870s-made many people think that our bodies possess some supernatural power. Mystics looked at this experiment as a support for some hazy teaching about the miraculous force emanating from the human body. Meanwhile the reason is natural and simple enough: the air heated from below by the hand moves upwards, pushing the paper and making it rotate, like the paper “snake” above a lamp discussed earlier. When you folded the paper, you made some of it slightly inclined. An acute observer will have noticed that the paper rotates in a definite direction, from the wrist along the palm to the fingers. This is explained by the difference in temperatures between parts of the hand: the finger tips are invariably colder than the palm, therefore the palm produces a larger upward current that strikes the paper stronger than that caused by the fingers. Does a Fur Coat Heat? What would you say if told that a fur coat doesn’t heat a bit? To be sure, you’d think the speaker is pulling your leg. And if this were proved by a number of experiments? For example, like the following. Record the reading of a thermometer and wrap it in a fur coat. Get it out several hours later. You’ll see that it hasn’t heated up by even a fraction of a degree, the reading will be as it was before. This proves that the fur coat doesn’t heat. You might suspect that fur coats even cool. Take two bottles with ice in them, wrap one 126-127 Seventy-Five More Questions and Experiments on Physics in the coat and allow the other to stand in the room uncovered. When the ice in the uncovered bottle has melted, unfold the fur coat and you’ll see that the ice is nearly intact. In consequence, the fur coat not only didn’t heat the ice, but, as it were, cooled it, thus hampering the melting!... What objections could be raised here? How could you refute the arguments? There is no objecting or refuting. In fact, fur coats don’t heat things up if by “heat up” we mean to impart heat. A lamp heats, a stove heats, a human body heats, too, because all of these bodies are sources of heat. But a fur coat is not. It generates no heat, but only stops the heat of our body from going astray. That’s why a warm-blooded animal whose body itself is a source of heat will be warmer with a fur coat than without it. But the thermometer generates no heat of its own and its temperature won’t change in the coat. The ice in the coat retains its low temperature longer because the fur coat-a fairly poor heat conductor-hinders the passage of heat from the outside. Snow “heats” the earth in the same way a fur coat does. A loose powder substance, snow is a poor heat conductor and helps to keep cold out. Not infrequently a thermometer in snow-covered soil indicates it is as much as ten degrees hotter than is exposed soil. Farmers are well aware of this heating effect of a snow cover. Thus, the answer to the question of whether a fur coat heats or not is that it only helps us to heat ourselves. Or rather we heat the fur coat, not vice versa. How to Air Rooms in Winter The best way to air a room is to open a window when a fire is burning. Fresh, cold outside air will then force out the warm, lighter air from the room into the fire-place and out through the chimney into the atmosphere. However, do not think that the same thing will occur when the window is closed, for the outside air will leak into the room through gaps in the window, walls, etc. True, some of it will really get into the room but not enough to sustain the fire. Therefore, apart from the outside air some air must come from other rooms where it might be neither pure nor fresh. The two accompanying figures demonstrate the difference between the two cases. The arrows indicate the flow of air. Where to Arrange a Ventilation Pane Where? At the top or bottom of a window? In some homes ventilation panes are at the bottom. Admittedly, these are convenient to open and close, but they are inefficient. Let’s consider the physics of the air exchange through the ventilation pane. Outside air is colder than that inside and displaces the latter. However, it occupies the part of the room below the ventilation pane. The air above the pane doesn’t contribute to the exchange, i. e. is not ventilated. Figure 96 Paper Saucepan Look at Fig. 96. An egg is being boiled in a paper vessel! You’d say, “Oh, but the paper'll now catch fire and the water will pour out!” Try the experiment on your own. Make the “saucepan” from parchment paper and attach it to a wire holder. The paper won’t be destroyed bythe fire. The reason is that water in an open vessel can only be heated to boiling temperature, i. e. 100 °C. Therefore, the water, which has a large thermal capacity, absorbs excess heat from the paper and so does not allow it to heat up more above 100° to a point when it might ignite. (Perhaps it would be more convenient to make use of a small paper box as shown in the figure.) So the paper does not catch fire although flames touch it. A similar kind, but disastrous, “experiment” is at 128-129 Seventy-Five More Questions and Experiments on Physics times performed by absent-minded people who put an empty kettle onto a fire with the pitiful result that the latter gets unsoldered. The reason is clear now: solder is relatively low-melting and it is only its close contact with water that saves it from its temperature. rising dangerously. This applies to all sorts of soldered things. Further, you could melt a piece of lead in a small box made of a playing card. You’ll only need to expose to flames the place that is in direct contact with the lead. Being a good heat conductor, the metal will quickly take away heat from the paper. The temperature of the paper will thus be maintained at about 335 °C (melting point for lead), which is insufficient to ignite the paper. What is the Lamp Glass for? Few people know what a long history the lamp glass went through before it appeared in its present-day form. For millennia people had used flames for lighting without resorting to the services of glass. It took the genius of Leonardo da Vinci (1452-1519) to introduce this important improvement of the lamp. But Leonardo used a metal tube, rather than a glass one, to surround the flame. Three more centuries passed before the metal tube was replaced by the transparent cylinder. You see thus that the lamp glass is an invention developed by scores of generations. What’s its purpose? Not all of you will come up with the right answer to this natural question. To protect the flames from wind is only a secondary role of the glass. Its main effect is to increase the brightness of the flames, to boost the combustion process. The role of the glass here is like that of a chimney or stack; it intensifies the inflow of air to the flames, i.e. improves the “draught”. Let’s take a closer look at this. The column of air inside the glass is heated by the flames much faster than the air surrounding the lamp. After it has heated and thereby become lighter, the air is displaced upwards by the heavier cold air arriving from below through holes in the burner. This results in a steady flow of air upwards, a flow that continually takes the combustion products out and brings fresh air in. The higher the glass, the more difference there is between the heated and unheated air columns and the more 9-621 Seventy-Five More Questions and Experiments on Physics intensive is the inflow of fresh air, and hence the burn¬ ing. The situation is like that in industrial chimney stacks which is why they are made so high. Interestingly, even Leonardo had understood these phenomena. In his manuscripts he says, “Where fire appears, an air flow forms around it, the flow supports and intensifies it.” Why Doesn't a Flame Go Out by Itself? A closer examination of the process of combustion inevitably leads to the above question. After all, the combustion products are carbon dioxide and water vapour, noncombustible substances incapable of supporting the process. Accordingly, once started a flame must be surrounded by noncombustibles that hinder the inflow of air. Combustion cannot occur without air and the flame would be bound to die out. Why then this is not the case? Why does the process of combustion carry on as long as there is a supply of combustibles? For the only reason that gases expand on heating and become lighter. It's owing to this that heated combustion products don’t stay where they’ve been formed, i.e. in the immediate neighbourhood of the flames, but are at once forced upwards by fresh air. If the principle of Archimedes didn’t apply to gases (or there were no gravity), any flame would go out after a while on its own. You can easily verify that combustion products kill a flame. At times you make use of this unawares to extinguish the fire in a lamp. How do you blow out a kerosene lamp? Blow into it from above, i.e. do not let the combustion products out. The flames go out deprived of the supply of fresh air. Why Does Water Kill Fire? A seemingly simple question... that is not always correctly answered. Let’s briefly explain the phenomenon. First, on touching a hot body water turns into vapour, so taking heat away from the burning body. To convert boiling water into vapour takes more than five times as much heat as is required to heat the same amount of cold water to 100 °C. Second, the resulting vapour occupies hundreds of times more space than the source water. The vapour 130-131 Seventy-Five More Questions and Experiments on Physics envelopes the body, cutting off the air that is indispensable for its burning. To improve the fire-extinguishing power of water they sometimes add ... gunpowder to it. Strange as it might seem, the measure is quite reasonable because the powder burns down quickly evolving a great amount of noncombustible gases that cover the burning material to hinder combustion. Heating with Ice and Boiling Water Is it possible to use a piece of ice to heat another? Or, to cool? Is it possible to heat one quantity of boiling water with another? If some ice at a low temperature, — 20 °C say, is brought into contact with a piece of ice at a higher temperature, — 5 °C say, then the first piece of ice will heat up (become less cold), and the second will cool down. Therefore, it is quite possible to cool or heat ice with ice. But one body of boiling water cannot heat another body of boiling water (at the same pressure), for at a given pressure boiling water is always at the same temperature. Can You Bring Some Water to the Boil Using Other Boiling Water? Pour some water into a small bottle (jar or phial) and place it in a saucepan with pure water so that it doesn’t touch the bottom. Of course, you’ll have to suspend the bottle from a piece of wire. Put the saucepan on a fire. When the water in the saucepan boils, it would seem that the water in the bottle should also boil shortly. Only you will never see this, however long you wait. The water in the bottle will get hot, very hot, but boil will it not. The boiling water appears to be too cool to bring another body of water to the boil. Quite an unexpected result, it seems, but let’s analyse it more closely. To bring water to the boil it is not sufficient only to heat it to I00°C-it also needs a substantial supply of so-called latent heat. Pure water boils at 100 °C, and under standard conditions its temperature never exceeds this, however long you heat it. In our case the source of heat used to heat the water in the bottle has a temperature of 100 °C. It, too, is 9* Seventy-Five More Questions and Experiments on Physics only able to heat the water in the bottle up to 100 °C. Once the 100 °C mark is reached in the bottle, any fur¬ ther transfer of heat from the water in the saucepan to that in the bottle will cease. No amount of heating can then supply the water in the bottle with the latent heat required for the water to vapourize (each gramme of water heated to 100 °C requires upwards of 500 calories* to vapourize). That’s why the water in the bottle, although it gets hot, doesn’t boil. A guestion may arise: what is the difference between the water in the bottle from that in the saucepan? After all, the bottle contains the same water except that it is only separated from the rest of the water by a glass partition. Now, why isn’t it involved in the processes occurring beyond the partition?Because the partition interrupts the currents that mix the water in the pan where each particle of water can directly touch the hot bottom. But the water in the bottle only contacts boiling water through the partition. Thus, pure boiling water cannot boil another amount of water. But just add a handful of salt to the saucepan... and everything changes. Salt water boils at somewhat higher than 100 °C and can thus bring the pure water in the bottle to the boil. Can You Bring Water to the Boil with Snow? The reader might answer, “If boiling water won’t do it how can snow!” Take your time to answer. You’d better carry out an experiment, say, with the bottle that you were just using before. Fill it halfway with water and insert it into boiling salt water. Wait for the water in the bottle to boil, take it out of the saucepan and plug quickly with a prepared well-fitting cork. Now turn the bottle upside-down and wait for the boiling inside to cease. Then pour boiling water over the bottle and the water inside won’t boil. But place some snow on its bottom or simply pour cold water over it, as shown in Fig. 97, and you’ll see that the water in the bottle will boil... The snow has done what the boiling water couldn’t. This is all the more mysterious because the bottle won’t be especially hot, only warm. But you will have * The calorie is a unit of heat. The small calorie is the amount of heat required to increase the temperature of 1 gramme of water by 1°C. 132-133 Seventy-Five More Questions and Experiments on Physics Figure 98 seen with your own eyes that the water in the bottle has boiled. The secret is that the snow cooled the walls of the bottle with the result that the vapour inside it condensed to form water droplets. Since the air has been expelled from the bottle before, the water inside the bottle is now under much lower pressure. But it’s well known that lowering the pressure of a liquid reduces its boiling point. Although in our bottle we have boiling water it’s not hot. If the walls of the bottle are very thin, the sudden condensation of vapour inside it can cause something like an explosion: the external pressure can squeeze the bottle (you see that the word “explosion” is unsuitable here and in fact what took place was an ‘implosion’). Instead of the bottle you’d better use a round vessel (a bulb with a convex bottom) so that external air would exert its pressure on the arch. It is safer to perform this experiment with a tin can used to contain kerosene, oil, etc. Boil some water in it, screw its plug on tightly and pour cold water over it. The can will at once collapse under the pressure of the external air as the vapour inside will condense into water on cooling. The can will be crumpled by atmospheric pressure as if hit by a heavy hammer (Fig. 98). A Hot Egg in Your Hand Why doesn’t an egg just out of boiling water hurt your hand? The egg is wet and hot. Water cools the shell on evaporating from the surface and the hand is not burned. But this only occurs in the first instants, until the egg has dried, and then its high temperature will hurt you. Removal of Fat Stains by an Iron The removal of fat stains from fabrics is based on the fact that the surface tension of liquids decreases with increasing temperature. “Therefore,” Maxwell wrote in The Theory of Heat, “if the temperature in various parts of the fat stain is different, the fat seeks to move from heated places to colder ones. Apply to one side of the fabric a heated iron, and to the other, cotton paper, the fat will then transfer to the cotton paper.” Seventy-Five More Questions and Experiments on Physics Accordingly, material absorbing the fat should be placed at the side opposite to the iron. How Far Can You See From High Places? From a flat place we only see the group up to a certain boundary. This boundary of view is called the “horizon line”. Trees, houses and other high structures lying beyond the horizon line are seen not in full, because their lower parts are blotted by the convexity of the earth. Even plains or the sea, although apparently flat, are in fact convex, for they are parts of the curved surface of the globe. How far then does an average-sized man see over a plain? He can only see up to 5 kilometres. To see beyond that he’ll have to climb up higher. A man on horseback on a plainland would see up to 6 kilometres and a sailor on a mast 20 metres high would see the sea around him up to 16 kilometres away. From the top of a lighthouse towering above water at 60 metres the sea is seen for nearly 30 kilometres. But, of course, the widest panoramas open up before airmen. From an altitude of 1 kilometre they can see almost for 120 kilometres in all directions, if not hindered by clouds or fog. At twice the height an airman will see for 160 kilometres using a perfect optical device. Further, from 10 kilometres one can see within 380 kilometres, and astronauts orbiting the Earth see the whole of one side of the globe. Where Does a Chirring Grass Hopper Sit? Sit somebody in the middle of a room, with his eyes blindfolded, and ask him to sit still and not turn his head. Take then two coins and tap one on the other at various places in the room but at about the same distance from your friend’s ears. Ask your friend to guess the place whence the sound comes. It will be diffi¬ cult to do and your friend will point in some other direction. If you step aside, the errors won’t be as bad because now the sound in the nearest ear of your friend will be heard somewhat louder, so enabling him to determine the location of the source. The experiment makes it clear why it’s impossible to spot a grass hopper chirring in the grass. The sharp 134-135 Seventy-Five More Questions and Experiments on Physics sound is heard two paces away from you. You look there and see nothing, but now the sound is distinctly heard from the left. You turn your head in that direction, but no sooner have you done that than the sound already comes from some other direction. The speed of the grass hopper stuns you and the quicker you turn to the direction of the singing insect the quicker the invisible musician hops about. But in reality the insect is sitting placidly in place and his “hops” are just an illusion. Your problem is that when you turn your head you put it exactly so that the grass hopper becomes equally separated from both of your ears. This condition (as you should know it from the experiment just described) is conducive to an error. If the chirring comes from ahead of you, you place it, erroneously, in the opposite direction. In consequence, if you want to determine where a sound comes from, you should not turn your head towards the sound, but conversely, turn it away. Which is exactly what we do when we, as it were, “prick up our ears”. Echo When a sound we have produced is reflected from a wall or another obstacle and returns to our ears, we hear an echo. It is only heard distinctly if the time-lag between the sound generation and its return is not too short. Otherwise the reflected sound would melt with the initial one and amplify it, the sound will then reverberate, e. g. in large empty halls. Imagine that you are standing in an open place and there is a house in front of you 33 metres away. Clap your hands. The sound will travel through the 33 metres, reflect from the walls and come back. How long will that take? Since the sound covered 33 metres there and the same distance back, it’ll return in 66/330 or 1/5 of a second. Our sharp sound was so short that it terminated in less than 1/5 second, i.e. before the echo arrived. The two sounds didn’t merge and were heard separately. A monosyllabic word (“yes”, “no”, etc.) is pronounced in about 1/5 second and we can hear such words echoed at a distance of only 33 metres from an obstacle. But for bisyllabicwords the echo merges with the initial sound intensifying it but rendering it obscure, we don’t hear it separately. At what distance must the obstacle be then so that Seventy-Five More Questions and Experiments on Physics we could hear a bisyllabic echo distinctly, “halloo”, say? Such words take 1/5 second to pronounce, during which time the sound should cover the distance to the obstacle and back, i. e. double the separation from the obstacle. But in 2/5 second sound covers 330 x 2/5 = = about 132 metres. A half of it-66 metres-is precisely the least distance to the obstacle capable of producing the bisyllabic echo. Now you’ll be able to work out that a trisyllabic echo requires a distance of about one hundred metres. Musical Bottles If you have ear for music, you could contrive a sort of a jazz band from conventional bottles and play simple tunes. What and how is to be done is evident from Fig. 99. Suspend 7 bottles with water from a pole fixed horizontally between two chairs. The first bottle should be nearly full, each successive bottle contains a little bit less water than the previous one, the last bottle having virtually none. By striking the bottles with a dry wooden stick you’ll produce various notes of the octave. The less water in a bottle the higher its pitch. Therefore, by adding or removing some water you’ll be able to achieve the tones that make up a scale. With an octave you could play some simple melodies on this bottle instrument. The Murmur in a Shell If you put a cup or a large shell next to your ear you’ll hear a murmur that occurs because the shell is a resonator that amplifies the numerous noises in the surrounding world that are not normally noticed because they are too weak. This mixed sound reminds people of the murmur of the sea and has led to numerous legends. 136-137 Seventy-Five More Questions and Experiments on Physics To See Through a Palm Fold a sheet of paper into a tube, bring it up to your left eye with your left hand and look through it at some distant object. Now bring your right palm near to your right eye so that it nearly touches the tube. Both hands should be about 15-20 centimetres away from the eyes. You’ll then make sure that your right eye sees perfectly through your palm as if there were a round hole in it. Why? The reason of this unexpected phenomenon was as follows. Your left eye prepared to view a distant object through the tube and the crystalline lens adapted accordingly. The eyes function in such a way that they always adapt in sympathy. In the experiment described the right eye, too, adapted to distant sight with the result that the near palm appeared blurred to it. In short, the left eye clearly sees the distant object, the right one, sees the palm unclearly. The net result is that it seems to you that the distant object is seen through the shielding palm. Through Binoculars At a seaside you are watching a boat approaching the shore through a pair of binoculars that magnifies three times. How many times will the speed be increased with which the boat is approaching the shore? Assume that the boat is sighted 600 metres away and is approaching the observer with a speed of 5 metres per second. Through binoculars with triple mag¬ nification the boat at 600 metres appears to be at 200 metres. A minute later it will be 5 x 60 = 300 metres closer and will then be 300 metres away from the observer. In the binoculars its apparent size would indicate it were 100 metres away. Consequently, an observer looking through the binoculars would think the boat has travelled 200 - 100 = 100 metres, whereas in actual fact it has actually covered 300 metres. It follows that the speed at which the boat approaches when observed through the binoculars has decreased not increased by three times. The reader can arrive at the same result by another argument, i.e. by taking the initial distance, speed and period. The speed with which the boat approaches has thus reduced by as many times as the binocular magnifies. Seventy-Five More Questions and Experiments on Physics From the Front or the Back? There are many things in each household that are used inefficiently. I’ve already mentioned that some people cannot use ice properly to chill drinks-they place them on the ice instead of under it. It appears that some people cannot use a conventional mirror either. Quite frequently, if they want to see themselves better in the mirror they turn the light on behind themselves in order to “illuminate the reflection”, instead of illuminating themselves from the front. Drawing Before the Mirror That a mirror reflection is not identical with the original may be demonstrated by the following experiment. Stand or hang an upright mirror in front of you on the table, place a sheet of paper on it and try to draw something, for example, a rectangle with diagonals. But in doing so don’t look directly at your hand, but follow the movements of its reflection in the mirror. You’ll find that this seemingly simple problem is almost intractable. Over the years our visual perceptions and motions have been correlated but the mirror violates this and represents our motions to our eyes in an inverted form. Long-term habits rebel against each our motion: you want to draw a line to the right, say, but the hand draws to the left, and so on. Stranger things will occur if instead of a simple figure you attempt to draw more intricate designs or write something whilst looking in the mirror. The result will be a funny confusion. The impressions left on carbon paper are inverted lettering, too. Just try to read the text on it. Quite a challenge! But bring it to a mirror and the text will appear in its habitual form. The mirror gives the reflection of what is itself an inverted image of normal writing. Black Velvet and White Snow Which is the lighter - black velvet on a sunny day or pure snow on a moonlit night? Nothing, it seems, surpasses black velvet in blackness or white snow in whiteness. These age-old metaphors of white and black appear, however, quite different when viewed by a physical instrument-a photometer. It then 138-139 Seventy-Five More Questions and Experiments on Physics turns out that the blackest velvet in sunlight is lighter than the purest snow in moonlight. This is because a black surface, however dark it might be, doesn’t completely absorb all the visible incident light. Even soot and platinum black-the blackest substances known-scatter about 1-2 per cent of the incident light. We take 1 per cent for argument’s sake and suppose that snow scatters 100 per cent of the incident light (which is undoubtedly an overstatement) *. It is known that the illumination provided by the sun is 400,000 times that of the moon. Therefore, the 1 per cent of sunlight scattered by the black velvet is thousands of times more intense than the 100 per cent of moonlight scattered by snow. In other words, sunlit black velvet is many times lighter than moonlit snow. To be sure, this is true not only of snow but also of the best white pigments (the whitest of them all-lithopone-scatters 91 per cent of light). Since no surface, unless it’s hot, can beam out more light than strikes it, and the sun sends out 400,000 times as much light as the moon, it’s impossible to have a white pigment that would in moonlight be lighter than the blackest pigment on a sunny day. Why is Snow White? Why, indeed? It consists of transparent ice crystals. For exactly the same reason that ground glass and all ground transparent substances in general are white. Grind some ice up in a mortar or chip it with a knife and you’ll get white powder. The colour is due to the fact that light, when penetrating into tiny pieces of transparent ice, doesn’t pass through them but reflects inside them at the boundaries between the ice and theair (total internal reflection). But a randomly scattering surface is perceived by the eye as white. Thus, snow is white because it consists of tiny particles. If the gaps between the snow flakes are filled with water, the snow becomes transparent. Such an experiment is easy. Put some snow into a jar and pour some water into it, and before your very eyes the snow will become colourless, transparent. * Fresh snow only scatters about 80 per cent of light. Seventy-Five More Quentions and Experiments on Physics The Shine on a Blackened Shoe Why does a blackened shoe shine? Neither the sticky black shoe polish, nor the brush seem to have anything to impart the gloss to shoes. Therefore, it’s a mystery for many. We’ll first clear up the difference between the glossy polished surface and the dull one. It’s widely believed that the polished surface is smooth and the dull one is irregular. This is not so: both are irregular. There are no absolutely smooth surfaces. Examined under the microscope polished surfaces would be like razor blades and for a man reduced 10,000,000 times the surface of a smoothly polished blade would appear to be a hilly terrain. There are irregularities, depressions and scratches on any surface, both dull and polished. What matters is the size of these irregularities. If they are smaller than the wavelength of the incident light, then the rays are reflected correctly, i.e. at the angle of incidence. Such a surface gives mirror reflections, it shines and we call it polished. If, on the other hand, the irregularities are larger than the wavelength of the incident light, the surface scatters the ray randomly and does not follow the reflection law. Such scattered light gives no mirror reflections and highlights, and the surface is called dull. This suggests, by the way, that a surface may be polished for some rays and dull for others. For visible light with a mean wavelength of about half a micrometre (0.0005 mm) a surface with irregularities of about that size will be polished; for infrared light, which has longer wavelength it’s polished, too. But for ultraviolet light, which has shorter wavelength, it’s dull. But back to the pedestrian subject of our problem. Why do polished shoes shine, after all? The unblackened surface of leather has a highly irregular microstructure with “peaks” larger than the mean wavelength of visible light, it’s dull. By blackening it we smooth out the surface and lay the hairs that stick out down. Brushing removes any excess polish at projections and fills the troughs, reducing the irregularities down to a size at which the peaks become smaller than the wavelengths of visible rays and the surface turns into a glossy one. 140-141 Seventy-Five More Questions and Experiments on Physics Through Stained Glass What colour are red or blue flowers viewed through green glass? Green glass will only transmit green light and catch all the rest. Red flowers send out mostly red light. If we look through green glass at a red flower we’ll receive no light from its petals as the only rays it emits are retained by the glass. The red flower will therefore appear to be black through such glass. Now you should easily see that the blue flower viewed through green glass will be black as well. Professor M. Yu. Piotrovsky, a physicist, artist and acute observer of nature, made a number of interesting observations in his book Physics on Summer Outings. “Observing flowerbeds through a red glass we see that purely red flowers, say, geranium, appear to us as bright as purely white one; green foliage appears as absolutely black with a metallic lustre; blue flowers (aconite, etc.) are so black as to be next to impossible to make them out against the black background of the leaves and yellow, pink, and lilac flowers appear more or less dull. “Through a green glass we see the unusually bright green of the foliage and white flowers come out still more distinctly against it; somewhat more pale are yellow and blue ones; red flowers are jet black; lilac and light-pink colours appear as dull and grey so that, for example, the light-pink petals of a wild rose are darker than its richly coloured leaves. “Finally a blue glass will again make red flowers look black, white flowers will look bright, yellow-absolutely black, and blue and dark-blue-almost as bright as the white ones. “It’s easily seen from this that red flowers really do emit much more red light than any other colour, yellow flowers emit about an equal amount of red and green, but very little blue, whilst pink and purple flowers emit a lot of red and blue, but very little green light.” A Red Signal On the railways the stop signal is a red colour. Why? Red light has the longest wavelength in the visible spectrum and is thus less scattered by any particles suspended in the air than are other colours. Therefore, red light penetrates farther. It is of paramount importance to obtain the greatest visibility possible for Seventy-Five More Questions and Experiments on Physics a transport signal since to be able to stop his train the engine-driver should begin breaking long before reaching an obstacle. The greater transparency of the atmosphere to longer waves, by the way, explains why astronomers use infrared filters to photograph planets (especially Mars). Fine details blurred in a conventional picture come out distinctly on a photograph taken through a glass that only transmits infrared light. In the case of Mars it’s possible to photograph the surface of the planet, while a conventional picture only shows its atmospheric envelope. A further reason for selecting the red light for the stop signal is that our eyes are more sensitive to this colour than to blue or green. Optical Illusions Tricks of Vision The optical, or visual, illusions to which this section is devoted are not- accidental companions of our vision-they occur in definite circumstances, are governed by physical laws and affect any normal human eye. That human beings are subject to visual illusions and can be mistaken as to the source of their visual perceptions, should by no means be considered an undesirable disadvantage or an unqualified flaw in our constitution, whose removal would benefit us in many respects. The artist would rebel against such an “infallible” vision. For him our ability, under certain conditions, to see what really is not is a blessing enriching enormously the potentialities of the fine arts. The 18th century mathematician Euler wrote: “Artists are especially skilled at using this common illusory experience. The whole of the art of painting is based on this. If we were used to judge about things as these are in reality then this art would be impossible, it would be as if we were all blind. In vain the artist would exhaust his skill in colour blending, for we would merely say: there is a red spot on this board, here a blue one, here a black and there, several whitish lines. Everything is in the same plane and there is no difference in distance. It would thus be impossible to represent anything. No matter what were painted in the picture, it could seem to be like writing on a paper, and perhaps we would, in addition, try to make out the signification of all the coloured spots. For all the perfection, weren't we to be pitied greatly, being devoid of the pleasure we derive every day from such pleasant and useful arts!" Since the subject is of such lively interest for the artist, physicist, physiologist, physician, psychologist, philosopher, and for any inquisitive mind, many books and articles have been published in this country and elsewhere. * We’ll here consider several types of tricks played by our unaided eye, i.e. without any appliances such as stereoscopes, punched cards, and so on. As to the causes of one or another visual illusion, only a relatively smalla two-pence piece, but how many times larger is it across?” I gave some thought to it-the glass was about four times wider than a two-pence. “Four times wider and the same thickness.” I went on to conclude, “The layer is only four times larger than a two-pence. The glass could only receive four coins, but you’ve already put in 15 and plan, it seems, to add some more. Where’s the room?” “Your calculation is wrong. If a ring is four times larger across than another, its surface area will be 16 times larger, not four.” “Well, I never!” “You should have known it. How many square centimetres are there in a square metre? One hundred?” “No, 100 times 100 which is 10,000.” “You see. With rings the same rule holds: if a ring is two times wider than another, it has four times the surface area, three times wider-nine times the area, four times wider-16 times the area, and so on. So, the By the Way volume of the buldge above the brim is 16 times larger than that of a two-pence piece. You see now where all the room is in the glass. It has even more room because the water can rise up about two two-pence pieces thickness.” “Could you really put 20 coins into the glass?” “Even more, if only you dip them carefully, without shaking.” “I wouldn’t ever have believed that a brimful glass could have enough room for so many coins.” I had to believe it though when I saw the heap of coins inside the glass with my own eyes. “Now, can you place 11 coins into 10 saucers so that there is only one coin in each saucer?” the brother asked. “Saucers with water?” “With or without water, as you please,” he laughed, setting 10 saucers in a row. “Another physics experiment?” “No, psychological. On with the job.” “Eleven coins in 10 saucers, and one in each... No, I can’t,” I gave up at once. “Go ahead, I’ll help you. We’ll place the first coin in the first saucer and the 11th as well, just for a time.” I did as he said, waiting in bewilderment. What is going to follow? “Two coins? Well, the third coin goes into the second saucer. The fourth into the third saucer, the fifth into the fourth, and so forth.” When I had placed the 10th coin into the ninth saucer I was surprised to see that the 10th saucer was vacant. Alex said, “Now that’s where we’ll place the 11th coin that we put tentatively into the first saucer.” He took the extra coin from the first saucer and placed it into the 10th saucer. Now 11 coins were lying in 10 saucers, one in each... Fantastic! Brother swiftly collected the coins not caring to explain the trick to me. “Just think. That’ll be both more interesting and more useful than getting ready-made solutions.” And ignoring my pleads he gave me a fresh problem. “Here are six coins. Arrange them in three rows so that there are three coins in each.” “That takes nine coins.” “Everyone can do it with nine. No, do it just with six.” 40-41 Figure 7 By the Way “Now again that’s something impossible.” “You’re too quick to give up. Look, it’s simple.” “There are three rows here, with three coins in each,” he explained. “But the rows criss-cross.” “Perhaps, but did I say that they mustn’t?” “If I’d known that this was allowed, I’d have guessed for myself.” “Well, then, guess how to solve the problem in another way. But not now, sleep on it. Here are three more problems in the same vein. The first one: arrange nine coins in ten rows with three coins in each. The second: arrange ten coins in five rows with four coins in each. The third problem is as follows. I draw a square divided into 36 smaller squares. Now try to arrange 18 coins with one in each small square so that in each row and column there are three coins... Aha, I’ve just remembered one more trick with coins. Take into one hand a 5 pence, into the other a 10 pence, but don’t tell me which coin is in which hand. I’ll figure it out. Only do the following mental arithmetic: double what’s in the right hand and treble what’s in the left, and then add the results. Ready?” “Yes.” “What’s the final result, odd or even?” “Odd.” “The 10 is in the right and the 5 in the left hand,” Alex proclaimed at once and was right on target. We repeated it once more. The result was even and my brother said without mistake that the 10 was in my left hand. “About this problem also think at leisure,” he said, “and finally. I’ll show you a fascinating game with counters. I’ve just made some counters by cutting out differently sized disks from a sheet of cardboard. The biggest counter is 5 centimetres in diameter, the next biggest 4 centimetres, and so on down to the smallest which is 1 centimetre in diameter.” By the Way He put three saucers side by side, and put a stack of counters onto the first saucer: so that the 5 counter went on the bottom on top of that was the 4 counter, and so on down to the 1 counter on top of the stack. “The whole stack of five counters is to be transferred onto the third saucer but you have to observe the following rules. Rule number 1: each time move 1 counter only. Rule number 2: never put a larger counter onto a smaller one. Rule number 3: counters may be placed temporarily onto the middle saucer but still observing the first two rules and the counters must end up on the third saucer in the initial order. The rules are simple as you can see. Now, go ahead.” I started. First I placed the 1 counter onto the third saucer, the 2 counter onto the middle one... and stopped. Where should the 3 counter go? It was larger than both the 1 and 2 counters. “Well, then,” my brother prompted, “Place the 1 onto the middle saucer, then the third saucer will be vacant for the 3. I did so. Now a further predicament. Where was I to place the 4? Accidentally, I hit upon an idea: first 1 transferred the 1 onto the first saucer, the 2 onto the third, and next put the 1 onto the third as well. Finally, after a long series of move I succeeded in transferring the 5 from the first saucer and ended up with the whole stack on the third saucer. “How many transfer did you make in all?” asked my brother okaying my job. “Didn’t count.” “Well let’s count then. After all, it’s interesting to find the least number of moves that could lead to the goal. If our stack included only two counters, not five, the 2 and the 1, how many moves would be required?” “Three: the 1 onto the middle saucer, the 2 onto the third one and then the 1 onto the third.” “Right. Add one more counter, the 3, and count how many moves you need to transfer the stack. We’ll proceed as follows: first we transfer the two smaller coins onto the middle saucer one after the other. This takes, as we already know, three moves. We then transfer the 3 onto the vacant third saucer-one more 42-43 By the Way move. Next we transfer both counters from the middle saucer, too, onto the third one-three more moves. The total is 3 + 1 + 3 = 7.” “For the four counters, let me count for myself. At first I transfer the three smaller counters onto the middle saucer-seven moves; then the 4 goes onto the third saucer-one move, and now the three smaller coins go onto the third saucer-seven more moves. Thus I get 7 + 1 + 7 = 15.” “Splendid. And for the five counters?” “15+1 + 15 = 31.” “Well, you got it right. But I’ll show you a way to simplify the procedure. Note that the numbers involved-3, 7, 15, 31-all represent the product of several twos minus one. Look!” And Alex wrote out the following table. 3 = 2 x 2-1 7 = 2 x 2 x 2-1 15 = 2x2x2x2-1 31 = 2x2x2x2x2-1 “I see, the number of the counters to be transferred equals the number of twos in the product. Now, I could calculate the number of moves for any stack of counters. For instance, for seven counters: it’s 2x2x2x2x2x2x2-l = 128-1 = 127. “You’ve thus mastered this ancient game. You need only know one practical rule which is if the stack contains an odd numbernumber have well established, * See, e.g. The Nature of Experience (1959) by R. Brain; Optical Illusions (1964) by S. Tolansky; The Neurophysiological Aspects of Hallucinations and Illusory Experience (1960) by W. Grey. Optical Illusions unquestionable explanations. These include those due to the structure of our eyes, irradiation, Mariotte's illusion (blind spot), astigmatism illusions, and so forth. As an instructive example we’ll consider the optical illusion of Fig. 141: white circles arranged in a certain way on a black background are perceived as hexahedrons. It seems to be well established that this kind of illusion is totally caused by so-called irradiation, i.e. the apparent expansion of light areas (which can be given a simple, clear physical explanation). “White circles expand due to irradiation and reduce the black gaps between them”. Professor Paul Bert writes in his Lectures on Zoology. He goes on to say that, “as each circle is surrounded by six other, it pushes adjacent ones on expanding and appears to be confined by a hexagon”. Suffice it to glance at the neighbouring figure (Fig. 141) where the same effect is observed for black circles against a white background for this explanation to be rejected: here irradiation only could reduce the size of black spots but could not change them into hexagons. For the two cases to be covered by the same principle the following interpretation might be suggest¬ ed. When viewing from a certain distance, the angle of vision of the gaps between the circles becomes smaller than a limit, so enabling their forms to be distinguish¬ ed. Each of the six neighbouring gaps then appears to be a straight line of a uniform thickness and the circles are thus bounded by hexagons. This interpretation also covers the paradoxical fact that at some distances white circles continue to appear to be round, whereas the black fringes around them have already assumed hexagonal forms. It’s only at larger distances that the hexagonal configuration is transferred from the fringe to the white spots. However, this explanation, too, is only a plausible assumption and, perhaps, there are several other possible explanations. It is necessary to prove that the possible cause is here the actual one. Most of attempts to explain individual illusions (except for the few mentioned above) are as unreliable and uncertain. Some tricks of vision still await their explanation. By contrast, others have too many explanations each of which would perhaps be sufficient in itself were there not so many additional ones that make it less convincing. Remember the famous illusion discussed since the time of Ptolemy-that of the increasing of the size of celestial bodies near horizon. 144-145 Optical Illusions No less than six possible theories, it seems, have been suggested, each of which has the only drawback that there are five more equally adequate explanations... Obviously, the entire domain of visual illusions is still in the pre-scientific stage of treatment and in need of establishing the basic methodology of its investigation. For want of any solid foundation in the form of relevant theories I have confined our discussion to the demonstration of unquestionable facts providing no explanations of what caused them and seeking only to present all the major types of visual illusion.* Only those involving portraits are explained at the end of the section since these are quite clear and incontestable... I also wanted to do away with some of superstitious notions that developed around this unique optical illusion. The series of illustrations opens with samples of illusions caused by clearly anatomical and physiological peculiarities of the eye. These are illusions due to the blind spot, irradiation, astigmatism, the retention of light impressions, and retina fatigue (see Figs. 100-107). In the blind spot experiment some of your field of vision may disappear in another way as well-as Mariotte did for the first time in the 18th century. The effect perhaps is even more striking. So Mariotte writes : “Against a dark background approximately at the level of my eyes I attached a small circle of white paper and at the same time asked someone to hold another circle beside the first one about 2 feet to its right but somewhat lower so that the image would strike the optical nerve of my right eye when I closed my left one. I stood next to the first circle and stepped back grad¬ ually without taking my right eye off it. When I was about 9 feet away, the second circle, which was about 4 inches across, completely disappeared from my field of vision. “I couldn’t ascribe it to its lateral position, as I could discern other things further to the side than it. I’d have thought it removed had I not been able to find it again with the slightest movement of my eye...”. These “physiological” tricks of vision are followed by a much larger class of illusions that are due to psycholo¬ gical reasons, which have not yet been sufficiently * The selection of illusions here is the result of many years of collecting. I’ve excluded, however, all those published illusions that have effect not on anybody’s eye or are not perceptible enough. 10-621 Optical Illusions Figure 100 clarified. It may perhaps be established that illusions of this kind are only the consequence of some preconceived erroneous judgement that is involuntary and subconscious in nature. The source of the misperception here is the mind, not the sensor. Kant aptly remarked, “Our senses deceive us not because they do not judge correctly, but because they do not judge at all”. Irradiation. When viewed from a distance the figures below-the circle and square-seem to be larger than those above, although they are equal in size. The larger the distance the more pronounced is the illusion. The phenomenon is called irradiation (see below). Figure 101 W y\ Irradiation. When viewed from a distance the figure with the black cross seems, owing to irradiation, to be distorted as shown in the accompanying figure on the right. Irradiation is due to the fact that each light point of an object produces on the retina of an eye not a point but a small circle because of so-called spherical aberration. Therefore a light surface on the retina is fringed by a light band that increases the place occupied by the surface. On the other hand, black surfaces produce reduced images because of the light band. The Mariotte Experiment. Close the right eye and look with the left one at the upper cross from a distance of 20-25 centimetres. You’ll notice that the middle, large white circle disappears completely, although the two smaller circles on either side are seen distinctly. If, with the same arrangement, you look at the lower cross, the circle only disappears in part. Figure 102 The phenomenon is caused by the fact that with this arrangement of the eye with respect to the figure the image of the circle falls on the so-called blind spot-the place insensitive to photic stimulation where the optic nerve is connected. 146-147 Optical Illusions Figure 103 X Figure 104 Figure 105 The Blind Spot. This experiment is a modification of the previous one. If you look at the cross at the right of the figure with your left eye at a certain distance you won’t see the black circle at all, although the two cir¬ cumferences will be seen. Astigmatism. Look at the lettering with one eye. Do all of the letters appear equally black? Normally one of the letters appears blacker than the rest of them. You need only to turn the page by 45° or 90° and some other letter will seem to be blacker. The phenomenon is explained by so-called astigmatism, i.e. different curvatures of the retina in different directions (vertical, horizontal, etc.). It’s only rarely that an eye is free of this imperfection. 10" Optical IllusionsFigure 106 Astigmatism. Figure 105 furnishes another way (cf. the previous illusion) of identifying astigmatism in an eye. If you bring the figure to the eye under examination (the other one being closed) you’ll notice at a certain, rather close, distance that two opposite sectors will seem blacker than the other two, which will appear grey. Figure 107 Figure 109 When viewing this figure, move it to the right and left and it’ll seem to you that the eyes in the figure swing horizontally. The illusion is accounted for by the eye’s property to retain visual perceptions for a short time after the stimulus has disappeared (cinema is based on this). Having concentrated on the white square at the top you’ll notice about half a minute later that the lower white line will have disappeared (owing to retina fatigue). The Muller-Lyer Illusion. The segment be seems to be longer than ab, although they are in fact equal. Figure 108 •If you rotate this figure (by turning the book) all the rings and the white toothed wheel will seem to be rotating, each about its own centre, in the same direction and with the same speed. 160-161 Figure 155 Optical Illusions On the left you see a convex cross, on the right-a concave one. But turn the book upside down and the figures will change their places. Actually the figures are identical, only they’re shown at different angles. Figure 156 Look at the photograph in Fig. 157 with one e>e 14-16 centimetres away from the centre of the picture. With this arrangement your eye will see the picture from the same point the objective of the camera "saw" 11-621 Optical Illusions Figure 157 Figure 158 X the scene. It’s this that accounts for the liveliness of the impression. The landscape acquires depth, the water glimmer. The eyes and the finger seem to point directly at you and follow you when you shift to the right or left. It has long been known that some portraits have the fascinating feature that they sort of follow the onlooker with their eyes and even turn their faces in his or her direction, wherever he or she shifts. This feature scares nervous people and is regarded by many as something supernatural. It has given rise to a number of superstitions and fantastic stories (e. g. The Portrait by Gogol). However, the explanation of this interesting illusion is very simple. Above all, the illusion is peculiar not only to portraits, but to other pictures, too. A gun drawn or photographed so that it is directed at the onlooker’" turns its muzzle in his direction when he moves to the right or left of the picture. Also, there is no evading a cart riding directly at the onlooker. All of these phenomena have one common and * Such a photograph is obtained if, in photographing, the muzzle of the gun is directed at the objective. In exactly the same way if the person being photographed looks into the objective, then his eyes in the picture will be directed at the onlooker, at whatever angle he views the picture. Optical Illusions the scene. It’s this that accounts for the liveliness of the impression. The landscape acquires depth, the water glimmer. The eyes and the finger seem to point directly at you and follow you when you shift to the right or left. It has long been known that some portraits have the fascinating feature that they sort of follow the onlooker with their eyes and even turn their faces in his or her direction, wherever he or she shifts. This feature scares nervous people and is regarded by many as something supernatural. It has given rise to a number of superstitions and fantastic stories (e.g. The Portrait by Gogol). However, the explanation of this interesting illusion is very simple. Above all, the illusion is peculiar not only to portraits, but to other pictures, too. A gun drawn or photographed so that it is directed at the onlooker’" turns its muzzle in his direction when he moves to the right or left of the picture. Also, there is no evading a cart riding directly at the onlooker. All of these phenomena have one common and * Such a photograph is obtained if, in photographing, the muzzle of the gun is directed at the objective. In exactly the same way if the person being photographed looks into the objective, then his eyes in the picture will be directed at the onlooker, at whatever angle he views the picture. 162-163 Optical Illusions exceptionally simple cause. If we view the picture we imagine the things shown in it, and it seems to us that the thing has changed its position. The same applies to the portraits. When we observe a real face from the side, we see another part of it. We can only see the same part as before if the person turns his face to us, but in a portrait we always see the same view. When a portrait is perfectly executed the effect is striking. Clearly, there is nothing surprising in this property of portraits. Conversely, it would be more unusual if, as we shift sidewards, we would see the side of the face. But, this, in essence, is what is expected by those who regard the apparent turn of the face in a portrait as something supernatural! Brain-Twisting Arrangements and Permutations In Six Rows You may have heard the funny story that nine horses have been put into 10 boxes, one in each. The problem that is now posed is formally similar to this famous joke, but it has a real solution'". You must arrange 24 people in six rows with five in each. In Nine Squares This is a trick question-half a problem, half a trick. Using matches make a square with nine small square cells and place a coin in each so that each row and column contain 6 kopecks (Fig. 159). The figure shows the arrangement of the coins. Place a match on one coin. Now ask your friends to change the arrangement without moving the coin with the match so that the rows and columns each still contain 6 kopecks. They’ll say it’s impossible. However, a small trick will help you to perform this “impossible” task. Which one? Coin Exchange Make a large drawing of the arrangement in Fig. 160 and denote each of the small squares by a letter in the top left corner as shown. Put 1 kopeck, 2 kopeck, and 3 kopeck coins into the three squares of the upper row. Now put 10 kopeck, 15 kopeck, and 20 kopeck coins into the three squares of the lower row. The rest of the squares are empty. By shifting the coins on vacant squares you make the coins exchange their places so that the 1 kopeck changes with the 10 kopecks, the 2 kopecks changes with the 15 kopecks, and the 3 kopecks with the 20 kopecks. You may occupy any vacant place of the figure but you are not permitted to place two coins into one square. Also, it isn’t allowed to skip an occupied square or go beyond the figure. The problem is solved by a long series of moves. Which moves? * In what follows the answers to problems are given at the end of each section. 164-165 Brain-1\visting Arrangements and Permutations Nine Zeros Nine zeros are arranged as shown below: 0 0 0 0 0 0 0 0 0 You must cross all the zeros with four lines only. To simplify the solution I will add that the nine zeros are to be crossed without the pencil leaving the paper. 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1 0 0 0 0 1 0 0 0 0 0 0 0 0 Thirty Six Zeros You see that 36 zeros are arranged in the cells of this network. You must cross out 12 zeros so that each row and column retain an equal number of uncrossed zeros. Which zeros are to be crossed? Two Draughtsmen Put two different draughtsmen on a draughts board. How many different arrangements are possible? Flies on a Curtain Nine flies are sitting on a chequered window curtain. They happened to have arranged themselves so that no two flies are in the same row, column, or diagonal (Fig. 161). Brain-Twisting Arrangements and Permutations After a while three flies shifted into neighbouring, unoccupied cells and the other six stayed in the same place. Curiously enough, the nine flies still continued to be arranged so that not a single pair appeared in the same direct or oblique line. Which three flies shifted and which cells did they choose? Figure 162 Figure 163 Eight Letters The eight letters arranged in the cells of the square shown in Fig. 162 are to be arranged in alphabetical order by shifting them into a vacant cell, as in the two previous problems. This is not difficult if the number of moves is not limited, but you are required to achieve the result using a minimum number of moves. You must find out for yourself what the minimum number is. Squirrels and Rabbits Figure 163 shows eight numbered stumps. On stumps 1 and 3 sit two rabbits, and on stumps 6 and 8, two squirrels. But both the squirrels and the rabbits are not happy with their seats and want to exchange them, the squirrelswant to take the places of the rabbits, and the rabbits the places of the squirrels. They can only make it by leaping from a stump to the other along the lines indicated in the figure. A 4 ? iv M 6 166-167 Brain- Twisting Arrangemen ts and Permutations How could they make it? Observe the following rules: (1) each animal may make several leaps at once; (2) two animals may not seat on the same stump, therefore they must only leap on a vacant stump. Further, you should take into account that the animals want to reach their goal using the least possible number of leaps, although it’s impossible to make less than 16 leaps. Cottage Problem Figure 164 The accompanying figure shows the plan of a small cottage whose poky rooms house the following furni¬ ture: a desk, a piano, a bed, a sideboard, and a bookcase. Only room 2 is free of furniture. The tenant wanted to change around the piano and the bookcase. This appeared to be a difficult problem because the rooms are so small that no two of the above pieces could be in the same room. The free room 2 was of help. By shifting the things from one room to another the desired arrangement was eventually achiev¬ ed. What is the least number of changes required to achieve the goal? Three Paths Three brothers-Peter, Paul, and Jacob-got three vegetable gardens located near their houses, as shown in the figure. You can see that the gardens are not very conveniently arranged but the brothers failed to agree about exchanging them. The shortest paths leading to the gardens crossed and the brothers began to quarrel. Wishing to avoid future conflict the brothers decided to find nonintersecting paths to their respective gardens. After a lot of searching they succeeded in finding such paths and now they come to their gardens without meeting each other. Could you indicate these paths? One requirement is that no path should go round Peter’s house. Brain-Twisting Arrangements and Permutations Pranks of Guards The following is an ancient problem having many modifications. We’ll discuss one of them. 168-169 Brain-Twisting Arrangements and Permutations The commander’s tent is guarded by sentries housed in eight other tents (Fig. 166) Initially in each of the tents there were three sentries. Later the sentries were allowed to visit each other and their chief didn’t punish them when, having come to a tent, he found more than three soldiers in it and less than three in the others. He only checked the total number of soldiers in each row of tents, thus if the total number of soldiers in the three tents of each row was nine, the chief thought that all of the guards were present. Having noticed this the soldiers found a way to outwit their chief One night four guards left and this passed unnoticed. On the next night six left and got away with that On later night the guards began to invite guests: at one time four, at another eight, and at yet another, a full dozen guests. And all of these pranks passed unnoticed as the chief always found nine soldiers in the three tents of each row. How did they manage to do so9 Ten Castles In olden days a prince desired to have 10 castles built. They should be connected by walls arranged on five straight lines with four castles on each. Tne architect submitted the plan given in Fig. 167 But the prince wasn’t satisfied with the plan because the arrangement made all the castles vulnerable to outside attack, but he wished there to be at least one or Figure 167 Brain-Twisting Arrangements and Permutations two castles protected within the walls. The architect objected that it was impossible to satisfy the condition whilst the 10 castles had to be arranged four in each of the five walls. But the prince insisted. After a lot of head-scratching the architect in the long run came up with an answer. Maybe you’ll be happy enough, too, to arrange the 10 castles and the five interconnecting walls so as to meet the above conditions? An Orchard There were 49 trees in an orchard, arranged as shown in Fig. 168. The gardener decided that the orchard was too crowded, so he wanted to clear the garden of excess trees to make flowerbeds. He called in a workman and ordered: “Leave only five rows of trees, with four trees in each row. Cut down the rest and take them home for firewood as your payment for the work”. When the tree felling had finished the gardener came 170-171 Brain-Twisting Arrangements and Permutations to see the result. Much to his dismay he found the orchard almost devastated: instead of the 20 trees the workman had left only 10 and cut 39. “Why have you cut so many? You were told to leave 20 trees!” the gardener was enraged. “No. You only told me to leave five rows with four trees in each. I did so. Just look.” The gardener was amazed to find that the 10 remaining trees formed five rows with four trees in each. His order had been fulfilled literally, and still... 39 trees had been cut down instead of 29. How had the workman managed it? The White Mouse All of the 13 mice in the figure are doomed to be eaten by the cat. But the cat wants to consume them in a certain order. TTie cat eats one mouse and then counts around the circle in the direction in which the mice are looking. When it gets to 13 it eats the mouse and starts counting again, missing out the eaten mice. Which mouse must it start from for the white mouse to be eaten last? Figure 169 Answers 6 In Six Rows The requirement of the problem is easily met if the people are arranged in the form of a hexagon as shown in the figure. Figure 170 In Nine Squares You don’t touch the forbidden coin but shift the whole of the lower row upwards (Fig. 171). The arrangement has changed but the requirement of the problem is satis¬ fied: the coin with the match hasn’t been shifted. 1 r "^T ©| Coin Exchange The following is the series of moves required (the number is the coin, the letter is the cell to which the coin is shifted): 2-e 15 — i 2-d 10-a 15-b 3-g 1-h 3-e 10-d 20-c 10-e 15-b 2-h 1 -e 2-j 2-d 20-e 3 -a 15 — i 3-j 10-j 15-b 3-g 2-i It’s impossible to solve the problem in less than 24 moves. 172-173 Answers Nine Zeros The problem is solved as shown in Fig. 172. Figure 172 Thirty Six Zeros As it’s required to cross out 12 of the 36 zeros, we’ll have 36 — 12, i.e. 24 zeros with four zeros in each row. The remaining zeros will be arranged as follows: »\i 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 o 1 0 Two Draughtsmen One draughtsman may be placed at any of the 64 squares of the board, i.e. in 64 ways, then the second one can occupy any of the 63 remaining squares. Hence for each of the 64 positions of the first draughtsman you can find 63 positions for the second one. Consequently, the total number of the various permutations of the two draughtsmen is: 64 x 63 = 4,032. Flies on a Curtain The arrows in Fig. 173 indicate which flies must be shifted and in which direction. Answers Figure 173 Eight Letters The least number of moves is 23. These are as follows: ABFECABFECABDHGABDHGDEF Squirrels and Rabbits Shown below is the shortest way of the rearrangement The first number in each pair indicates from which stump an animal should leap and the second number the destination stump (for example, 1-5 means that a squirrel has leapt from the first stump to the fifth). The total number of leaps required is 16, namely: 1-5; 3-7; 7-1; 5-6; 3-7; 6-2; 8-4; 7-1; 8-4; 4-3; 6-2; 2-8; 1-5; 5-6; 2-8; 4-3. Cottage Problem The exchange can be achieved in no less than 17 moves. The pieces of furniture are moved in the following sequence: 1. Piano 7. Piano 13. Bed 2. Bookcase 8. Sideboard 14. Sideboard 3. Sideboard 9. Bookcase 15. Table 4. Piano 10. Table 16. Bookcase 5. Table 11. Sideboard 17. Piano 6. Bed 12. Piano Three Paths The threenonintersecting paths are shown in Fig. 174. 174-175 Answers Peter's house Figure 174 Jacob's garden Peter's garden Paul's garden Pranks of Guards The problem is easily solved by the following reasoning. For four guards to be able to be absent unnoticed by the chief it’s necessary that in rows / and III (Fig. 175a) there are nine soldiers in each. As the total number is 24 — 4 = 20, then in row II there will Figure 175 IV V^ VI '□□□ 000 000 omo “'□□□ 000 000 a b c 000 000 □ 0□ 0B0 0*0 000 000 000 d e f be 20 — 18 = 2, i.e. one soldier in the left tent of this row and one in the right. In the same way we find that there must be one soldier in the upper tent of row V and one in the lower. It is now clear that the comer tents must house four guards. Accordingly, the required arrangement for four soldiers to be absent is as shown in Fig. 1756. A similar argument yields the desired arrangement for six soldiers to be absent (Fig. 175c). For four guests the arrangement is shown in Fig. 175J; For eight guests in Fig. 175c; And finally, Fig. 175/ shows the arrangement for 12 guests. It is easy to see that under these conditions no more than six soldiers can be absent with impunity and no more than 12 guests can visit the guards. Ten Castles Figure 176 (on the left) shows the arrangement with two castles protected from the external attack. You see that the 10 castles are disposed as required in the problem: Answers Figure 176 four on each of the five lines. On the right of Fig. 176, four more solutions to the problem are given. An Orchard The uncut trees were disposed as given in Fig. 177. These form five straight rows with four trees in each. Figure 111 176-177 Answers The White Mouse The cat should first eat the mouse at which it is looking, i. e. the sixth one from the white. Try it by beginning with this mouse and cross out every 13th mouse. You’ll see that the white mouse will be the last to be crossed out. Skilful Cutting and Connecting With Three Straight Lines Figure 178 Figure 179 Cut Fig. 178 into seven sections with three straight lines so that there is one animal in each section. Into Four Parts This ground area (Fig. 179) consists of five equal squares. Draw the area on a sheet of paper. Can you cut it into four identical areas, not five? To Make a Circle Figure 180 A joiner was given two pieces of rare wood with holes in them (as shown) and was asked to make them into a perfectly circular solid board for a table so that no scraps of the expensive wood would be left over. All the wood must be used. The joiner was a master craftsman but the order was not easy. He scratched his head for a long time, tried one way and then another, and eventually hit upon an idea as to how to execute his order. Perhaps you’ll twig it, too? Cut out two paper figures, exactly like the ones in Fig. 180 (only larger) and use them to arrive at the solution. A Clock Dial The clock dial in Fig. 181 must be cut into six parts of any shape so that the sum of numbers in each section 178-179 Skilful Cutting and Connecting Figure 181 would be the same. The aim of the problem is not so much to test your resourcefulness but the quickness of your thought. Crescent The crescent (Fig. 182) must be divided into six parts by only two straight lines. To Divide a Comma In the accompanying figure you will see a wide comma. It’s constructed very simply: a semicircle is drawn on the straight line AB around point C, then two semicircles are drawn around the middles of the segments AC and CB, one on the right, the other on the left. You must cut the figure into two identical parts by a single curved line. The figure is also interesting in that two such figures make up a circle. How? To Develop a Cube If you cut a cardboard cube along edges so that it could be unfolded and placed with all six squares on a table, you’ll get a figure like one of those shown in Fig. 184. Figure 184 It’s curious, but how many different figures can be obtained in this way? In other words, in how many ways can a cube be developed? I warn the impatient reader that there are no less than 10 different ways. To Make Up a Square Can you make up a square from five pieces of paper like the ones shown in Fig. 185a? If you’ve already found the solution, try and make up Skilful Cutting and Connecting a square from five identical triangles like the ones you have just used (the base is twice as long as the height). You may cut one of the triangles into two parts but the other four must be used as they are (Fig. 185t). 180-181 Answers 7 With Three Straight Lines The problem is solved as follows: Figure 186 Into Four Parts The dash lines show the way in which the ground must be divided (Fig. 187). Figure 187 To Make a Circle The joiner has cut each of the boards into four parts as shown on the left of Fig. 188. From the four smaller parts he makes up a smaller inner circle to which he glues the other four parts. He thus got an excellent board for a round table. Figure 188 Answers A Clock Dial As the sum of all the numbers on the face of the dial is 78, the sum of each of the six sections must be 78-^6 = 13. This facilitates finding the solution that is shown in Fig. 189. Figure 189 Crescent The answer is shown in the accompanying figure. The resultant six parts are numbered. To Divide a Comma The solution is seen in the accompanying drawing. Both parts of the comma are equal, as they are made up of equal parts. The figure shows how the circle is made of two commas, one white and one black. l ... Figure 191 _ ; — ■ | Ly To Develop a Cube All the 10 possible solutions are shown in Fig. 192. The first and fifth figures can be turned upside down and this will add two more involutes, increasing the total to 12. 182-183 Answers Figure 192 / Id T * 3 To Make Up a Square The solution of the first problem is shown in Fig. 193a. The case of triangles is given in Fig. 193k One triangle is first cut up as shown. Figure 193 Figure 194 Problems with Squares A Pond There is a square pond (Fig. 194) with four old oaks growing at its comers. It is required to expand the pond so that its surface area be doubled, the square shape being retained and the old oaks not destroyed or swamped. A Parquet Maker When cutting wooden squares a parquet maker tested them thus: he compared the lengths of sides and if all four sides were equal he considered the square to be cut correctly. Is this test reliable? Figure 195 Another Parquet Maker Another parquet maker checked his work otherwise: he measured diagonals not the sides. If both diagonals were equal, he considered the square to be true. Are you of the same opinion? Yet Another Parquet Maker Yet another worker checked his squares by seeing if all the four sections into which the diagonals divide each other (Fig. 195) are equal to each other. In his opinion it proved that the rectangle cut was square. What do you make of that? 184-185 Problems with Squares A Seamstress A seamstress wants to cut out a piece of linen in the form of a square. Having cut several pieces she checks her work by bending each piece along its diagonal to see if the edges coincide. If they do, she thinks, each piece is perfectly square. Is she right? Another Seamstress Another seamstress wasn’t satisfied with the check her companion used. She bent her piece first along one diagonal and then after smoothing the linen she bent it along the other. It was only if the edges of the piece coincided in both cases that she thought the square was correct. What would you say about this test? A Joiner's Problem Figure 196 A young joiner has the five-sided board shown in Fig. 196. You see that it seems to be composed of a square glued to a triangle that is four timessmaller than the square. The joiner is asked to make the board into a square, taking nothing away from the board and adding nothing to it. This, of course, involves cutting it into sections. Our young joiner is just going to do so, but he wants to cut the board along no more than two straight lines. Is it possible, using two lines, to cut the figure into parts from which the joiner could make a square? And if the answer is “yes” how does he go about it? Answers A Pond It is possible to double the surface area of the pond with the square shape retained and the oaks intact. The accompanying figure shows how this can be done. You can Figure 197 easily see that the new area is twice the earlier, just draw in the diagonals of the earlier pond and count the resultant triangles. A Parquet Maker The test is not sufficient. Some quadrilaterals that are by no means squares will pass. Figure 198 gives examples of quadrilaterals whose sides are equal but whose angles are not right (rhombs). Figure 198 Another Parquet Maker This test is as unreliable as the first one. To be sure, a square’s diagonals are equal but not every quadrilateral with equal diagonals is a square. It is clearly seen from the examples in Fig. 199. Figure 199 The parquet makers should apply both tests to each quadrilateral produced. One could then be sure that the work has been done correctly. Any rhomb with equal diagonals is bound to be a square. 186-187 Answers Yet Another Parquet Maker The test might only show that the quadrilateral in question has right angles, i. e. that it is a rectangle. But it fails to verify that all its sides are equal, as is seen in Fig. 200. Figure 200 A Seamstress The test is far from adequate. Figure 201 presents several quadrilaterals whose edges coincide when bent along the diagonals, yet they are not squares. You see how far Figure 201 /\ /7 /\ a quadrilateral may differ from a square and still satisfy this test. The test only shows that the figure is symmetrical, no more. Another Seamstress This test is no better than the previous one. You could cut any number of quadrilaterals out of paper that would pass this test, although they are by no means squares. The examples in Fig. 202 all have equal sides (these are rhombs) but the Figure 202 angles are not right-hence these are not squares. In order to make really sure that the pieces cut out are squares, the seamstress should additionally check if the diagonals (or angles) were equal. A Joiner's Problem One line should go from the vertex c to the middle of side de, the other, from the last point to vertex a. A square can be made up from the three pieces 1, 2, and 3 as shown in Figure 203. c Figure 203 Problems on Manual Work Navvies Five navvies excavate a 5-metre ditch in 5 hours. How many navvies are required to dig 100 metres of ditch in 100 hours? Lumberjacks A lumberjack cuts a 5-metre log into 1-metre lengths. If each cut takes 1.5 minutes, how long will it take to cut the log? Joiner and Carpenters A team of six carpenters and a joiner did a job. Each carpenter earned 20 roubles, but the joiner got 3 roubles more than the average earnings of all the seven team members. How much did the joiner earn? Figure 204 Five Pieces of Chain A blacksmith was given five pieces of chain with three links in each (Fig. 204) and asked to connect them. The blacksmith opened and reclosed four links. But is it not possible to do the same job with fewer links tampered with? How Many Vehicles? A shop repaired 40 vehicles (cars and motocycles) in a month. The total number of wheels on the vehicles was 100. How many cars and motocycles were repaired? Potato Peeling Two people peeled 400 potatoes. One completed three pieces a minute, the other two. The second worked 25 minutes longer than the first. How long did each work? Two Workers Two workers can perform a job in seven days provided the second starts two days later than the first. If the job 188-189 Problems on Manual Work were done by each of them separately, then the first would take four days more than the second. How many days would each of them take to perform the job individually? The problem permits of a purely arithmetic solution without any need to manipulate fractions. Typing a Report Two typists type a report. The more experienced one could finish the work in 2 hours, the other in 3 hours. How long will it take them to do the job if they divide it so as to spend the least time possible? Problems of this kind are normally solved according to the procedure of the famous problem on reservoirs. Thus in our problem they would find the share of the work done by each typist, add up the fractions and divide unity by the resultant sum. Could you think of some other procedure? Weighing Flour A salesman has to weigh five bags of flour. His problem was that the shop had a balance but some weights were missing so that it was impossible to weigh from 50 to 100 kilogrammes. But the bags weighed 50-60 kilogrammes each. The man began to weigh the bags in pairs. Of the five bags it is possible to make 10 different pairs, so he had to make 10 weighings. He produced the series of numbers given below in the ascending order: 110 kg, 112 kg, 113 kg, 114 kg, 115 kg, 116 kg, 117 kg, 118 kg, 120 kg, 121kg. How much did each bag weigh? Answers x \_J' Navvies It’s easy to swallow the bait and think that if five navvies dug 5 metres of the ditch in 5 hours, then it would take 100 people to dig 100 metres in 100 hours. But that argument is absolutely wrong, since the same five navvies would be required, no more. In fact, five navvies dig 5 metres in 5 hours, so they can do 1 metre in 1 hour, and in 100 hours-100 metres. Lumberjacks The common answer would be 1.5 x 5, i.e. 7.5 minutes. That is because many people often forget that the last cut will give two 1-metre lengths. Thus, it’s only necessary to cut the log four times, not five, and this will take 1.5 x 4 = 6 minutes. Joiner and Carpenters We can easily find the average earnings of a member of the team by dividing the extra 3 roubles between the six carpenters. Accordingly, we should add 50 koppecks * to the 20 roubles earned by each carpenter to arrive at the average earnings of each of the seven workers. We’ll thus obtain that the joiner earned 20 roubles 50 kopecks plus 3 roubles, i. e. 23 roubles 50 kopecks. Five Pieces of Chain It’s only necessary to open the three links of one of the pieces and to use the links obtained to connect the other four pieces. How Many Vehicles? If all the 40 vehicles were motocycles, the total number of wheels would be 80, i. e. by 20 less than in reality. Replacing a single motocycle by a car increases the total number of wheels by two and the difference decreases by two. Clearly, 10 such replacements are required for the difference to be reduced to zero. So, there were 10 cars and 30 motocycles. In fact: 10 x 4 + 30 x 2 = 100. Potato Peeling During the 25 extra minutes the second peeler put out 2 x 25 = 50 pieces. We subtract 50 from 400 to find that if the two had worked an equal time they would have yielded 350 potatoes. As their production per minute was 2 + 3 = 5 pieces, then by dividing 350 by 5 we find that each would have worked for 70 minutes. 1 rouble = 100 kopecks. Answers 190-191 This is the actual duration of work of the first peeler, the second one worked for' 70 + 25 = 95 minutes. In fact: 3 x 70+2 x 95 = 400. Two Workers If each worker performs half the job individually, the first would need two days more than the second (because the difference in duration for the whole job is four days). As in our case the difference is just two days when the two work together, it is then obvious that during the seven-day period the first worker performs half the job, whereas the seconddoes his half in five days. Thus, the first worker would be able to do the whole job himself in 14 days and the second in 10 days. Typing a Report A nonstereotyped approach is as follows. First, we’ll ask the question: if the typists are to finish the work simultaneously, how should they divide it? (Clearly, it’s only under this condition, i. e. without any time wasted, that the work will be done in the shortest time possible). As the more experienced typist types 1.5 times faster it’s obvious that her share should be 1.5 times larger than that of the other if both are to stop simultaneously. It follows that the first typist should take over three fifths of the report, and accordingly the second two fifths. As a matter of fact the problem is nearly solved. It only remains to find the time taken by the first typist to do her share of the job. We know she can do the whole job in 2 hours, hence the three fifths of the job will be carried out in 2 x 3/5 = 11/5 hours. During exactly this time the second typist will finish her share of the job. Thus, die shortest time required for both typists to type the report is 1 hour and 12 minutes. Weighing Flour To begin with, the salesman summed up the 10 numbers. The resultant sum (1,156 kilogrammes) is nothing but the fourfold weight of the bags: the weight of each bag enters the sum four times. If we divide .by four, we’ll find that the total weight of the five bags is 289 kilogrammes. We’ll now for convenience assign numbers to the bags in ascending order of their weights. The lightest bag will be No. 1, the second No. 2, etc., and the heaviest. No. 5. It will be seen that in the series of quantities: 110 kg, 112 kg, 113 kg, 114 kg, 115 kg, 116 kg, 117 kg, 118 kg, 120 kg, and 121 kg, the first quantity is the sum of the weights of the two lightest bags. No. 1 and No. 2; the second quantity, of No. 1 and No. 3. The last quantity (121) is the sum of the two heaviest bags, No. 4 and No. 5, and the penultimate, of No. 3 and No. 5. Thus: No. 1 and No. 2 give 110 kg No. 1 and No. 3 » 112 kg No. 3 and No. 5 » 120 kg No. 4 and No. 5 » 121 kg Answers We can thus easily find the sum of the weights of No. 1, No. 2, No. 4, and No. 5: 110 kg + 121 kg= 231 kg. Subtracting this number from the total weight of the bags (289 kg) gives the weight of No. 3, namely - 58 kg. Further, from the sum of No. 1 and No. 3, i.e. from 112 kg, we subtract the now-known weight of No. 3 to arrive at the weight of No. 1: 112 — 58 = 54 kg. In exactly the same way we find the weight of No. 2 by subtracting 54 kg from 110 kg, i.e. from the sum of No. 1 and No. 2. The weight of No. 2 will thus be 110 — — 54 = 56 kg. Now from 120 kg (No. 3 + N0. 5) we subtract the weight of No. 3 (58 kg) to get the weight of No. 5: 120—58 = 62 kg. It remains to determine the weight of No. 4, knowing the sum of No. 4 and No. 5 (121 kg). Subtracting 62 from 121 gives that No. 4 weighs 59 kg. The weights of the bags are thus 54 kg, 56 kg, 58 kg, 59 kg, 62 kg. We have solved the problem without any resort to equations. 192-193 Problems on Purchases and Prices How Much are the Lemons? Three dozen lemons cost as many roubles as one can have lemons for 16 roubles. How much does a dozen lemons cost? Raincoat, Hat and Overshoes A raincoat, hat and overshoes are bought for 140 roubles. The raincoat costs 90 roubles more than the hat, and the hat and the raincoat together cost 120 roubles more than the overshoes. How much does each thing cost separately? Use mental arithmetic only, no equations. Purchases When I went out shopping I had in my purse 15 roubles in 1 rouble pieces and 20 kopeck coins. When back home I had as many 1 rouble pieces as there had been 20 kopeck coins initially, and as many 20 kopeck coins as I had had 1 rouble pieces initially, my purse only containing a third of the initial sum. How much had I spent? Buying Fruit One hundred pieces of various fruit can be bought for five roubles. The prices are: water-melons, 50 kopecks a piece; apples, 10 kopecks a piece; and plums, 10 kopecks a ten. How many fruit of each kind are bought? Prices Up and Down The price of a product first went up 10%, and then down 10%. When was the price lower, initially or finally? Barrels Six barrels of beer were shipped to a shop. The numbers in Fig. 205 show the numbers of litres in each barrel. Two customers bought five of the six barrels, Problems on Purchases and Prices one bought two and the other bought three. Given that the second bought twice as much beer as the first, which barrel wasn’t sold? Selling Eggs At first sight, this ancient problem might seem incon¬ gruous as it involves selling half an egg. Nevertheless, it’s quite solvable. A peasant woman came to a market to sell some eggs. A first buyer took half her eggs plus 1 /2 of an egg. A second buyer bought half the remaining eggs plus another 1/2 of an egg. A third only bought one egg, which was the last. How many eggs were there initially? Benediktov's Problem Many experts in Russian literature don’t suspect that the poet V. G. Benediktov (1807-1873) was also the author of the first collection of mathematical brain-twisters in the language. The collection wasn’t printed and remained in a manuscript form to be found only in 1924. I had the opportunity to get acquainted with the manuscript and even established, based on one of the problems, the year it was compiled, namely 1869 (the manuscript wasn’t dated). The problem given below has been treated by the poet and named “An Ingeneous Solution of a Difficult Problem”. “An egg seller sent her three daughters to the market with ninety eggs. She gave ten to the eldest and 194-195 Problems on Purchases and Prices cleverest daughter, thirty to the second, and fifty to the third, saying: ‘You should agree beforehand on the price at which you’ll sell the eggs and stick to it. All of you should adhere to this price but I hope that the eldest daughter who is so bright will nevertheless be able to get as much for her ten eggs as the second daughter will receive for her thirty and she will teach the second sister how to get as much for her thirty as the youngest sister will get for her fifty eggs. Let the takings and prices be the same for the three of you. Furthermore, I’d like you to sell the eggs so that on average you will receive no less than 10 kopecks for ten, and no less than 90 kopecks for the ninety!”’ Here I interrupt Benediktov’s story so that the readers could figure it out for themselves how the girls went about their business. Answers IQ How Much are the Lemons? We know that the 36 lemons cost as many roubles as they sell lemons for 16 roubles. But 36 lemons cost 36 x (price of one lemon). For 16 roubles one can have 16/(price of one lemon). Hence, 36 x (price of one lemon) = 16/(price of one lemon). After some algebra we have (price of one lemon) x (price of one lemon) = 16/36. Clearly, one lemon costs 4/6 = 2/3 rouble and a dozen lemons cost 2/3x12 = 8 roubles. Raincoat, Hat and Overshoes If instead of the raincoat, hat, and overshoes only two pairs of overshoes were bought, the price would be not 140 roubles, but 120 roubles less. Thus, the two pairs of overshoes cost 140 — 120 = 20 roubles, hence one pair cost 10 roubles. Now we find that the raincoat and the hat together cost 140 — 10 = 130 roubles, the raincoat costing 90 roubles more than the hat. We argue as earlier: instead of the raincoat and hat we could buy two hats, and we would pay not 130 roubles but 90 roubles less, i.e. 130 — 90 = 40 roubles. Hence one hat costs 20 roubles. Thus, the prices of the things were as follows: the overshoes-10 roubles, the hat-20 roubles, and the raincoat-110 roubles. Purchases Denote the initial number of 1 rouble pieces by x, and the number of 20 kopeck coins by y. Then when I went out shoppingI had in my purse (lOOx + 20y) kopecks. Back from my shopping expedition I had (lOOy + 20x) kopecks. As stated, the latter sum is three times smaller than the former, hence 3 (lOOy + 20x) = lOOx + 20y. Rearranging the expression gives x = ly. If y = 1, then x = 7. Under this assumption I initially had 7 roubles 20 kopecks Answers 196-197 which is at variance with the statement of the problem (“about 15 roubles”). Let’s try y = 2, this gives x = 14. The initial sum is thus 14 roubles 40 kopecks which checks well with the problem statement. The assumption of y = 3 leads to an overestimation: 21 roubles 60 kopecks. In consequence, the only fitting answer is 14 roubles 40 kopecks. When I returned back from my shopping excursion I only had two 1 rouble pieces and fourteen 20 kopeck coin, i. e. 200 + 280 = 480 kopecks, which actually amounts to a third of the initial sum (1,440/3 = 480). As I spent 1,440 — 480 = 960 kopecks, my purchases had cost 9 roubles 60 kopecks. Buying Fruit Despite the seeming uncertainty the problem has the only solution: Number Cost Water melons 1 50 kopecks Apples 39 3 roubles 90 kopecks Plums 60 60 kopecks Total 100 5 roubles 00 kopecks Prices Up and Down It would be erroneous to consider that the two prices are equal. It’s easily shown that this is not the case. After the price went up the article cost 110%, or 1.1 of the initial price. But after the price went down it amounted to 1.1 x 0.9 = 0.99, i.e. 99% of the initial price. Consequently, the final price was 1% lower than the initial one. Barrels The first customer bought the 15 litre and 18 litre barrels and the second-the 16 litre, 19 litre and 31 litre barrels. Really, 15+18 = 33 16 + 19 + 31 = 66, i. e. the second customer bought twice as much beer as the first one. The 20 litre barrel remained unsold. This is the only possible solution as no other combination gives the relationship required. Selling Eggs The problem is worked out backwards from the end. After the second buyer bought half the remaining eggs plus 1/2 of an egg, there was only one egg that remained with the peasant woman. Accordingly, 11/2 eggs was half of what remained after the first Answers 70 ® sale and so the full number is three eggs. We add 1/2 of an egg to obtain half of what the woman had initially. Thus, the woman had brought seven eggs for sale. Let’s check: 7/2 = 3 1/2; 3 1/2+1/2 = 4; 7 — 4 = 3 3/2 = 1 1/2; 1 1/2 + 1/2 = 2; 3 - 2 = 1, which complies with the conditions of the problem. Benediktov's Problem We continue the interrupted story: “The problem was a very difficult one. The sisters put their heads together on their way to the market, the two younger sisters seeking advice of the eldest. The latter gave some thought to the matter and said: ‘Sisters, we’ll sell the eggs not by the ten, as is the custom here, but by the seven. And we’ll set a price for the seven we’ll stick to as Mother said. Not a kopeck down from the set price! The first seven goes for three kopecks, agreed? ‘Dirt-cheap’, the second sister said. ‘But’, the eldest sister continued, ‘we’ll raise the price for those eggs that’ll remain after we have sold the full sevens. I’ve checked beforehand that there’ll be no other egg sellers in the market. No one to beat down the price. But when there is demand and the supply is dwindling the price rises. So we’ll make up for our loss with the remaining eggs’. ‘And what will we charge for the remaining eggs?’ the youngest sister asked. ‘Nine kopecks for each egg. Cash down! Those who need eggs badly will pay’. ‘Rather dear,’ the second sister noted again. ‘What of it?’ the eldest said, ‘the first eggs will have been sold cheaply by the seven. One will compensate for the other!’ “Understandably, the first to go were the fifty eggs of the youngest sister. She received 21 kopecks for 7 sevens and one egg remained in her basket. The second one sold 4 sevens for 12 kopecks and two eggs remained in her basket. The eldest sister sold a seven for 3 kopecks and three eggs remained in her basket. “The last six eggs were sold for nine kopecks each. So the eldest got 27 kopecks for her three eggs which brought her takings to 30 kopecks. The second sister got 18 kopecks for her last pair of eggs which when added to the 12 kopecks received earlier for her 4 sevens, gave her 30 kopecks as well. The youngest sister got 9 kopecks for her single egg and when she added the money to the 21 kopecks for her 7 sevens her total was 30 kopecks, too. “Thus, the money they got for ten appeared to be equal to the money they got for fifty.” 198-199 Weight and Weighing One Million Times the Same Product A product weighs 89.4 grammes. Figure out how many tonnes a million of them weigh. Honey and Kerosene A jar of honey weighs 500 grammes. The same jar filled with kerosene weighs 350 grammes. Honey is twice as heavy as kerosene. What is the weight of the empty jar? A Log A round log weighs 30 kilogrammes. How much would it weigh if it were twice as thick, but twice as short? Under Water Consider a balance on the one pan of which there is a boulder that weighs exactly 2 kilogrammes and on the other, an iron weight of 2 kilogrammes. I carefully immerse the balance in water. Will the pans be in equilibrium? A Decimal Balance A decimal balance weighs 100 kilogrammes of iron nails that are balanced by iron weights. When submerged, will the balance be in equilibrium? Figure 206 A Piece of Soap Onto one pan of a balance a piece of soap was put, onto the other 3/4 of a same sized piece plus 3/4 kilogramme. The balance is in equilibrium. What is the weight of a whole piece? Try and solve the problem mentally, without a pencil and paper. Cats and Kittens The accompanying figure shows that the four cats and three kittens together weigh 15 kilogrammes and that Weight and Weighing Figure 207 Figure 208 three cats and four kittens weigh 13 kilogrammes. All the cats have the same weight, so do the kittens. How much does one cat weigh? And a kitten? This problem, too, should be solved mentally. Shell and Beads Figure 208 shows that three children’s blocks and one shell are balanced by 12 beads and further that one shell is balanced by one block and eight beads. How many beads should be placed on the vacant pan for the shell on the other pan to be balanced? Figure 209 Fruit A further problem of the same kind. It is seen in Fig. 209 that three apples and one pear weigh as much as 10 peaches, but six peaches and one apple weigh as much as one pear. How many peaches are required to balance one pear? How Many Glasses? You see in Fig. 210 that a bottle and a glass are balanced by a jug, the bottle is balanced by a glass and a saucer, and two jugs are balanced by three saucers. How many glasses should be placed on the vacant pan for the bottle to be balanced? With a Weight and a Hammer It’s required to weigh out 2 kilogrammes of sugar into 200-gramme packets. There is, however, only one Weight and Weighing 200-201 500-gramme weight and hammer that weighs 900 grammes. How should one go about it using the weight and the hammer? Archimedes’s Problem The most ancient of brain-twisters pertaining to weighing is undoubtedly the one the tyrant of Syracuse Hieron gave to the famous mathematician Archimedes. The legend has it that Hieron entrusted a craftsman to manufacture a crown for a statue and ordered to give him the required amount of gold and silver. When it was ready, the crown weighed as much as the initial amounts of gold and silver had originally weighed together, but the craftsman was alleged to have stolen some of the gold having replaced it by silver. Hieron called in Archimedes and asked him to determine how much gold and silver respectively the crown contained. Archimedes solved the problem proceeding fromthe fact that in water pure gold loses one twentieth of its weight, and silver one tenth. If you want to try your hand at the problem suppose that the craftsman was given 8 kilogrammes of gold and 2 kilogrammes of silver and when Archimedes weighed the crown under water the result was 9 1/4 kilogrammes, not 10 kilogrammes. Given that the crown was made of solid metal, without any voids, how much gold had the craftsman stolen? Answers One Million Times the Same Product The mental arithmetic here is as follows. We must multiply 89.4 grammes by one million, i.e. by one thousand thousands. We can do the multiplication in two steps: 89.4 x 1,000 = 89.4 kilogrammes because the kilogramme is 1,000 times larger than the gramme. Then, 89.4 kilogrammes x x 1,000 = 89.4 tonnes, because the tonne is 1,000 times larger than the kilogramme. The weight we seek is thus 89.4 tonnes. Honey and Kerosene Since honey is twice as heavy as kerosene, the difference in weight (500 — 350= 150 grammes) is the weight of the kerosene in the volume of the jar (the jar of honey weighs as much as a jar containing a double aipount of kerosene). Hence we determine the weight of the jar: 350— 150 = 200 grammes. Really: 500 — 200 = 300 grammes, i.e. the honey is two times heavier than the same amount of kerosene. A Log A common answer is that a log, whose thickness has increased twice, and length decreased twice, should be the same weight. This is not so, however. Doubling the diameter increases the volume of a round log fourfold, but halving its length halves its volume. The net result is that the final log is twice as heavy as the initial one, i.e. it weighs 60 kilogrammes. Under Water Each immersed body becomes lighter by the weight of the water displaced by it. This law, discovered by Archimedes, will help us to answer the problem. The 2-kg boulder has a larger volume than the 2-kg iron weight because the material of the boulder (granite) is lighter than iron. Accordingly, the boulder will displace a larger volume of water than the weight and, according to Archimedes’s principle, loses more than the weight. The weight will thus outweigh the boulder under water. Decimal Balance When immersed in water, an iron object loses one eighth of its weight.* Thus both the nails and the weights will when immersed have only 7/8 of their former weight. Since the weights were 10 times lighter than the nails before immersion and they continue to be 10 times lighter after immersion, the equilibrium will not be disturbed. * The figure wasn’t given in the statement of the problem as the exact share of the weight lost is immaterial here. 202-203 Answers A Piece of Soap Three quarters of a piece of soap plus 3/4 kilogrammes weigh as much as the whole piece. But a whole piece is 3/4 plus 1/4, hence 1/4 of a piece weighs 3/4 kilogrammes and the whole piece weighs four times as much as 3/4 kilogrammes, i. e. 3 kilogrammes. Cats and Kittens A comparison of both weighings shows that replacing a cat by a kitten reduces the weight by 2 kilogrammes. It follows that a cat is 2 kilogrammes heavier than a kitten. With this in mind we in the first weighing replace all the four cats by kittens to obtain 4 + 3 = 7 kittens that will together weigh not 15 kilogrammes but 2x4 = 8 kilogrammes less. Consequently, the seven kittens weigh 15 — 8 = 7 kilogrammes. Hence a kitten weighs 1 kilogramme, and a cat weighs 1 + 2 = 3 kilogrammes. Shell and Beads Compare the first and second weighings. You’ll see that in the first weighing the shell can be replaced by one cube and eight beads. We’ll then have four cubes and eight beads on the left pan balanced by 12 beads. If we now remove eight beads from each pan, we won’t upset the balance. There’ll four cubes now remain on the left pan, and four beads on the right. One cube thus weighs the same as one bead. We can now work out the weight of the shell: replacing (second weighing) the cube on the right pan by a bead gives that the weight of the shell is equal to that of nine beads. The result can be checked easily. In the first weighing, replace the cubes and shell on the left pan by an appropriate number of beads. You’ll thus obtain 3 + 9=12, as required. Fruit In the first weighing we replace one pear by six peaches and an apple. We may do so because the pear weighs as much as the six peaches and apple. We then obtain four apples and six peaches on the left pan and 10 peaches on the right. Removing the six peaches from each pan gives that the four apples weigh as much as four peaches. Accordingly one peach weighs the same as one apple. Now it’s easy to figure out that a pear weighs the same as seven peaches. How Many Glasses? The problem has several different solutions. The following is just one of them. In the third weighing we replace each jug by a bottle and a glass (we know from the first weighing that the balance should remain in equilibrium). We thus find that two bottles and two glasses are balanced by three saucers. It thus appears that four glasses and two saucers are balanced by three saucers. Removing two saucers from each pan shows that four glasses are balanced by one saucer. Hence one bottle is balanced (compare with the second weighing) by five glasses. Answers With a Weight and a Hammer The procedure to be followed is like this. First put the hammer on one pan and the weight on the other. Then add just enough sugar for the pans to be in equilibrium. It’s clear that the sugar weighs 900 — 500 = 400 grammes. The operation is performed three more times. The remaining sugar weighs 2,000 — (4 x 400) = 400 grammes. It is only remains now to halve each of the five 400-gramme packets obtained. It’s a straightforward exercise: the contents of a 400-gramme packet are divided between two packets put on different pans until the balance balances. Archimedes's Problem If the crown ordered had been made purely of gold, it would have weighed 10 kilogrammes in air losing when immersed 1/20 part of its weight, i. e. 1/2 kilogramme. But we know that in fact the crown lost in water 10 — 9 1/4 = 3/4 kilogramme, not 1/2 kilogramme. This was because it contained silver-a metal that in water loses 1/10 part of its weight, not 1/20 part. The crown thus contained an amount of silver sufficient for it to lose in water 3/4 kilogramme, rather than 1/2 kilogramme, i.e. 1/4 kilogramme more. Suppose in the purely golden crown one kilogramme of gold were replaced by silver, the crown would when immersed lose another 1/10-1/20 = 1/20 kilogramme. Consequently, in order to decrease the crown’s weight by 1/4 kilogramme it was necessary to replace with silver as many kilogrammes of gold as there were l/20ths in 1/4: 1/4^ 1/20 = 5. So, the crown contained 5 kilogrammes of silver and 5 kilogrammes of gold instead of the 2 kilogrammes of silver and the 8 kilogrammes of gold the craftsman was given. Thus, 3 kilogrammes of gold had been stolen and replaced by silver. 204-205 Problems on Clocks and Watches 12 Three Clocks In my home there are three clocks. On the 1st of January they all showed true time. But only the first clock kept perfect time, the second was a minute slow a day, and the third was gaining a minute a day. Should the clocks continue like this, how long would it take for them all to show true time again? Two Clocks Yesterday I checked my wall clock and alarm clock and set them correctly. The wall clock is 2 minutes slow an hour, the alarm clock gains 1 minute an hour. Today both clocks stopped simultaneously since they had run down. The wall clock shows 7 o’clock and the alarm clock 8 o’clock. At what time yesterday did I set the clocks? Figure 212 What Time Is It? “Where are you hurrying to?” “To catch the 6 o’clock train. How long have I got left?” “50 minutes ago there were four times more minutes after three.” What does this strange answer mean?What time was it? When Do the Hands Meet? At 12 o’clock one hand is above the other. But you may have noticed that it is not the only moment when the hands meet: they do so several times a day. Can you say when all those moments are? When are the Hands Pointing in Opposite Directions? By contrast, at 6 o’clock both hands point in opposite directions. But is it only at 6 o’clock that this is the case or there are some other such moments during the next 12 hours? Problems on Clocks and Watches On Either Side of Six O'Clock I glanced at a clock and noticed that both hands were equally separated from 6. What time was it? The Minute Hand Ahead of the Hour Hand When is the minute hand as far ahead of the hour hand as the hour hand in turn is ahead of the figure 12 on the face? And maybe there are several such moments during the day or none at all? Vice Versa If you observe a clock attentively, you may have noticed the reverse arrangement of the hands as compared with that just described: viz. the hour hand is as far ahead of the minute one as the minute hand is ahead of the figure 12. When does this happen? Three and Seven A clock strikes three. And while it does so 3 seconds elapse. How long does it take the clock to strike seven? I warn you, just in case, that this isn’t a joke, i. e. it’s not a trick question. Ticking Lastly, make a small experiment. Put your watch on a table, move a few steps aside and listen to the ticking. If it’s sufficiently quiet in the room, you’ll hear that your watch sounds, as it were, in intervals: ticks for a while, then is silent several seconds, and then starts ticking again, and so on. Explain! 206-207 Answers 12 Three Clocks 720 days. During this time the second clock will lose 720 minutes, i.e. exactly 12 hours, and the third clock will have gained exactly the same time. Then all the three clocks will show as they did on the 1st of January, i.e. true time. Two Clocks The alarm clock is gaining 3 minutes an hour compared with the wall clock. Thus it gains an hour, i.e. 60 minutes, every 20 hours. But during these 20 hours the alarm clock gains 20 minutes compared with true time. This implies that both clocks were set correctly 19 hours 20 minutes before, i.e. at 11.40. What Time Is It? Between 3 and 6 o’clock there are 180 minutes. The number of minutes to go to 6 o’clock is easily found by dividing 180 — 50 = 130 minutes into two parts, one of which being four times larger than the other. Hence, we’ll have to find 1/5 part of 130. It was thus 26 minutes to 6 o’clock. In fact, 50 minutes before it was 26 + 50 = 76 minutes to go to 6 o’clock. Accordingly, 180 — 76 = 104 minutes had passed since 3 o’clock, which is four times longer than the time to go to 6 o’clock. When Do the Hands Meet? We start our observation at 12 o’clock, when both hands meet. Since the hour hand moves 12 times slower than the minute one (it takes 12 hours to make a complete circle, and the minute one 1 hour), the hands cannot, of course, meet during the next hour. But after the hour has passed and the hour hand come to the 1 o’clock mark (having completed 1/12th of the full circle), the minute hand has made a complete turn and is again at 12, i.e. 1/12 part of the circle behind the hour hand. The condition of the race is now different since the hour hand moves slower than the minute one, but is ahead of the minute hand which has to overtake it. If the race lasted an hour, the minute hand would have gone round a complete circle, and the hour hand 1/12 part of the circle, i.e. the minute hand would have travelled 11/12 part of the circle more. But to overtake the hour hand, the minute hand must only cover 1/12 of the circle which is the distance separating them. This requires a period of time that is the same fraction of an hour as 1/12th is a fraction of 11/12 i.e. one eleventh. Thus, the hands will meet in 1 /11 hour, i. e. in 60/11 = 5 5/11 minutes. The hands will thus meet 5 5/11 minutes after the first hour has elapsed, i.e. at 5 5/11 minutes past one. What about the next meeting? You should be able to see that it’ll occur 1 hour 5 5/11 minutes later, i.e. at 10 10/11 minutes past 2 o’clock. The next meeting occurs another 1 hour 5 5/11 minutes later, i.e. at 16 4/11 minutes past 3 o’clock, and so forth. You may have already guessed that, all in all, there’ll be 11 such meetings. The 11th comes 1 1/11x11 = 12 Answers hours after the first one, i.e. at 12 o’clock. In other words, it coincides with the first meeting, with future meetings occurring at the previous times. Let’s list the times of all the meetings: 1st-5 5/11 minutes past 2nd-10 10/11 minutes past 3rd-16 4/11 minutes past 4th—21 9/11 minutes past 5th—27 3/11 minutes past 6th-32 8/11 minutes past 7th-38 2/11 minutes past 8th-43 7/11 minutes past 9th-49 1/11 minutes past 10th-54 6/11 minutes past 11th- 1 o’clock 2 o’clock 3 o’clock 4 o’clock 5 o’clock 6 o’clock 7 o’clock 8 o’clock 9 o’clock 10 o’clock 12 o’clock When Are the Hands Pointing in Opposite Directions? The approach here is very much like that in the previous problem. We’ll again begin at 12 o’clock when both hands meet. We want to find the time required for the minute hand to get ahead of the hour hand by exactly half a circle, it is then that the hands are pointing in opposite directions. We already know (see the previous problem) that during an hour the minute hand gets ahead of the hour hand by 11/12 part of the circle. For it to get ahead by only 1/2 a circle takes less than an hour by so many times as 1/2 is less than 11/12, i.e. 6/11 part of an hour. Accordingly, after 12 o’clock the first time the hands point in opposite directions is in 6/11 hours, or 32 8/11 minutes. Look at a watch at this time and you’ll see that the hands are really pointing in opposite directions. Is this the only moment when we have such an arrangement? Of course, not. The hands are so arranged 32 8/11 minutes after each meeting. We already know that during a 12 hour’s time there are 11 such meetings. Hence the hands point opposite ways 11 times every 12 hours. These moments are easily found: 12 o’clock+ 32 8/11 minutes = 32 8/11 minutes past 12 o’clock 1 o’clock 5 5/11 minutes+ 32 8/11 minutes = 38 2/11 minutes past 1 o’clock 2 o’clock 10 10/11 minutes+ 32 8/11 minutes = 43 7/11 minutes past 2 o’clock 3 o’clock 16 4/11 minutes + 32 8/11 minutes = 49 1/11 minutes past 3 o’clock, and so on. I leave it for you to find the remaining moments. On Either Side of Six O’Clock The problem is solved like the previous one. Imagine that both hands are at 12 and that the hour hand has shifted by a certain part of a circle to be denoted by x. Meanwhile the minute hand has turned by 12x. If the time that has passed is less than one hour, then to meet the conditions of our problem the minute hand must travel a full circle less the angle covered by the hour hand since 12. In other words, 1 - 12x = x. Hence 1 = 13x and x = 1/13 part of a circle. The hour hand covers this fraction of Answers 208-209 a circle in 12/13 part of an hour, i.e. when it is (12/13) x 60 minutes or 55 5/13 minutes past 12 o’clock. During the same period of time, the minute hand covers 12 times more, i.e. 12/13 part of a circle. You see that both hands are equally separated from 12, and hence equally separated from 6, too. We’ve found one location of the hands, namely one that comes about in the first hour. During the second hour this occurs once more and you can find it arguing along the same lines as before, from the relation 1 — (12x — 1) = x or 2 — 12x = x. Hence 2= 13x and x = 2/13 of a circle. So the hands will be in the right position at (1 11/13) x 60 minutes or at 50 10/13 minutes past 1 o’clock. The hands will meet our requirement next time when the hour hand has shifted 3/13 of a circle away from 12, i.e. at 2 10/13of counters the first counter is transferred onto the third saucer, if its’s even, it goes onto the middle saucer.” “You say it’s an ancient game, didn’t you invent it yourself?” “No, I only applied it to counters. But the game as such has a very ancient origin and apparently came from India where there is a marvellous legend associated with it. It says that in the town of Benares is a sanctuary into which the Indian god Brahma, as he was creating the world, installed three diamond sticks and put on one of them 64 golden rings with the largest at the bottom and each of the rest being smaller than the one beneath it. The priests of the sanctuary were obliged ceaselessly to transfer these rings from one stick to another using the third as an auxiliary and observing the rules of our game that is to move one ring at a time By the Way and not to place it onto a smaller one. The legend has it that when all the 64 rings have been transferred the end of the world will come.” “Oh, it means the world should’ve perished long ago!” “Perhaps, you think transferring 64 rings won’t take much time?” “Of course. Allowing a second per move, you can make 3600 transferrings in an hour.” “Well.” “And about 100,000 in 24 hours. In 10 days, a million moves. A million would be enough, I think, to transfer even a thousand, not 64 rings.” “You are mistaken. To handle the 64 rings would take as much as 500,000,000,000 years!” “But, why? After all, the number of moves is only equal to the product of 64 twos, which amounts to...” “‘Only’ upwards of 18,000,000,000,000,000,000.” “Wait a bit, I’ll now multiply and check.” “Splendid. While you do your multiplying, I’ll have time to go to tend to my business,” said brother and left. I first found the product of 16 twos, then multiplied the result by itself. A tedious job, but I was patient and worked it out to the end. I obtained the number 18,446,744,073,709,551,616. Thus my elder brother was right... I mustered up courage and set about the problems he had set to me to solve on my own. They didn’t turn out to be all that difficult, some were even rather easy. The business of 11 coins in 10 saucers appeared ridiculously simple: we put the first and eleventh coins into the first saucer, next we put the third coin into the second saucer, the fourth coin into the third saucer, and so forth. But what about the second coin? It was ignored and that was the trick. The idea behind guessing which hand had the 10 pence coin was also simple. Doubling 5 gives an even number but trebling it gives an odd one 44-45 By the Way Figure 11 whereas multiplying 10 always gives an even number. Therefore, if the total was even, then the 5 had been doubled, i. e. it must have been in the right hand, and if the total was odd, it is clear that the 5 must have been trebled, i.e. been in the left hand. The solutions to the problems on the coin arrangements are clear from the accompanying drawings (Fig. 10). Finally, the problem with coins in the small squares works out as shown in Fig. 11. The 18 coins are arranged in the square with 36 small squares and giving three coins in each row. Wandering in a Maze Wandering in a maze • People and rats • Right- and left-hand rule • Mazes in ancient times • Tournefort in a cave • Solution of the maze problem. “What are you laughing at in your book? A funny story?” Alex asked me. “Yes, it’s Three Men in a Boat by Jerome.” “I remember it had me in stitches! Where are you?” “Where the crowd of people is wandering about in a garden maze, looking for a way out.” “An interesting story. Read it again for me, please.” So I read the story aloud from the very beginning: “Harris asked me if I’d ever been in the maze at Hampton Court. He said he went in once to show By the Way somebody else the way. He had studied it up in a map, and it was so simple that it seemed foolish-hardly worth the twopence charged for admission. Harris said he thought that map must have been got up as a practical joke because it wasn’t a bit like the real thing, and only misleading. It was a country cousin that Harris took in. He said: ‘We’ll just go in here, so that you can say you’ve been, but it’s very simple. It’s absurd to call it a maze. You keep on taking the first turning to the right. We’ll just walk round for ten minutes, and then go and get some lunch.’ “They met some people soon after they had got inside, who said they had been there for three-quarters of an hour, and had had about enough of it. Harris told them they could follow him, if they liked; he was just going in, and then should turn round and come out again. They said it was very kind of him, and fell behind, and followed. “They picked up various other people who wanted to get it over, as they went along, until they had absorbed all the persons in the maze. People who had given up all hopes of ever getting either in or out, or of ever seeing their home and friends again, plucked up cour¬ age, at the sight of Harris and his party, and joined the procession, blessing him. Harris said he should judge there must have been twenty people following him, in all; and one woman with a baby, who had been there all the morning, insisted on taking his arm, for fear of losing him. “Harris kept on turning to the right, but it seemed a long way, and his cousin said he supposed it was a very big maze. ‘“Oh, one of the largest in Europe,’ said Harris. “‘Yes, it must be, replied the cousin, because we’ve walked a good two miles already.’ “Harris began to think it rather strange himself, but he held on until, at last, they passed the half of a penny bun on the ground that Harris’s cousin swore he had noticed there seven minutes ago. Harris said, ‘Oh, impossible!’ But the woman with the baby said, ‘Not at all,’ as she herself had taken it from the child, and thrown it down there, just before she met Harris. She also added that she wished she never had met Harris, and expressed an opinion that he was an impostor. That made Harris mad, and he produced his map, and explained his theory. “‘The map may be all right enough, said one of the 46-47 By the Way party, if you know whereabouts in it we are now.’ “Harris didn’t know, and suggested that the best thing to do would be to go back to the entrance, and begin again. For the beginning again part of it there was not much enthusiasm; but with regard to the advisability of going back to the entrance there was complete unanimity, and so they turned, and trailed after Harris again, in the opposite direction. About ten minutes more passed, and then they found themselves in the centre. “Harris thought at first of pretending that that was what he had been aiming at; but the crowd looked dangerous, and he decided to treat it as an accident. “Anyhow, they has got something to start from then. They did know where they were, and the map was once more consulted, and the thing seemed simpler than ever, and off they started for the third time. “And three minutes later they were back in the centre again. “After that they simply couldn’t get anywhere else. Whatever way they turned brought them back to the middle. It became so regular at length, that some of the people stopped there, and waited for the others to take a walk round, and come back to them. Harris drew out his map again, after a while, but the sight of it only infuriated the mob, and they told him to go and curl his hair with it. Harris said that he couldn’t help feeling that, to a certain extent, he had become unpopular. “They all got crazy at last, and sang out for the keeper, and the man came and climbed up the ladder outside, and shouted out directions to them. But all their heads were by this time, in such a confused whirl that they were incapable of grasping anything, and so the man told them to stop where they were, and he would come to them.o’clock, and so on. All told, there are 11 such positions, the hands changing sides after 6 o’clock. The Minute Hand Ahead of the Hour Hand If we start looking at a clock at 12 o’clock exactly, then during the first hour we won’t see the position desired. Why? Because the hour hand covers 1/12 part of what the minute hand does, and hence lags behind the minute hand far more than is required for the arrangement we seek. Whichever the angle through which the minute hand turns about 12, the hour hand will only be at 1/12 part of that angle, not a half as is desired. But suppose an hour has elapsed and the minute hand is at 12 and the hour hand at 1, i.e. 1/12 part of a complete turn ahead of the minute hand. Let’s see if such an arrangement of the hands may come about during the second hour. Suppose that die moment has come when the hour hand has turned by a fraction of a circle that we’ll denote by x. Meanwhile the minute hand has covered 12 times more, i.e. 12x. If now we subtract from this a complete turn, the difference 12x — 1 must be twice as large as x, i.e. 2x. Thus 12x — 1 = 2x, whence it follows that a complete turn equals lOx (because 12x— 10x = 2x). But if lOx equals a complete turn, then lx = 1/10 part of a turn. We’ve thus arrived at the solution: the hour hand must have moved by 1/10 part of a turn past 12 o’clock. This takes 12/10 hours or 1 hour 12 minutes. The minute hand will then be two times farther away from 12, i.e. at 1/5 of a turn away, which corresponds to 60/5 = 12 minutes, as required. We’ve found one solution to the problem. But there are other ones and during a period of 12 hours the hands come to be arranged in the right way several times. We’ll try to find the other solutions. To find the next time we’d have to wait till 2 o’clock and now the minute hand is at 12 and the hour hand at 2. Reasoning along the same lines as before we arrive at 12x — 2 = 2x, whence two complete turns are equal to lOx, and hence x = 1/5 part of a complete turn. This corresponds to the moment 12/5 = 2 hours 24 minutes. I leave it to you to work out further moments. You’ll find that the hands arrange themselves in the right way at the following 10 instants in time: 1.12 7.12 2.24 8.24 14-621 Answers 3.36 9.36 4.48 10.48 6.00 12.00 The answers “6.00” and “12.00” might appear wrong, but only at first sight. In fact, at 6 o’clock the hour hand is at 6 and the minute one, at 12, i. e. exactly twice as far. At 12 o’clock the hour hand is separated from 12 by “zero” and the minute one, if you wish, by “double zero” (because double zero is just zero). So, this case, too, meets the restrictions of our problem. Vice Versa After the treatment we have just given, this problem is an easy exercise. Using the same arguments as above we can determine that for the first time the required arrangement will occur at the time given by 12x — 1 = x/2. Therefore 1 = 11 1/2 x, or x = 2/23 of a turn, i.e. (2/23) x 12 hours or 1 1/23 hours after 12 o’clock. Hence at 2 14/23 minutes past 1 o’clock the hands will be arranged correctly. The minute hand will then be midway between 12 o’clock mark and 1 1/23 hours mark, i.e. at 12/23 hours mark, which is exactly 1/23 part of a turn (the hour hand will be at 2/23 part of a turn). The hands will be arranged in the required manner for the second time at a time which can be found from the relation 12x — 2 = x/2. It follows that 2=11 1/2 x and x = 4/23, the time we seek is 5 5/23 minutes past 2 o’clock. The third moment is 7 19/23 minutes past 3 o’clock, and so forth. Three and Seven The commonest answer is “7 seconds”. But, as we’ll now see, that is wrong. When the clock strikes three we have two gaps: (1) between the first and second strokes, (2) between the second and third strokes. Each gap thus lasts 1 1/2 seconds. But when the clock strikes seven, there are six such gaps, which gives 9 seconds. Ticking The enigmatic interruptions in the ticking are only due to fatigue in your ears. From time to time your perception of sound becomes blunted for a second or two so that in these intervals you won’t hear the ticking. This aural fatigue passes off after a short while and previous ability to perceive the sound returns with the result that you again hear the ticking. Then another fatigue period comes on, and so forth. Problems on Transport A Plane's Flight An aircraft covers the distance from town A to town B in 1 hour 20 minutes. However, it takes it 80 minutes to get back. How could you explain it? Two Locomotives You may have seen a train driven by two locomotives, one at the front and the other at the back. But have you ever given any thought as to what happens to the couplings between the carriages and to their bulfers? The front locomotive only pulls the carriages when the coupling is taut, in which case the bulfers do not press against each other and so the rear locomotive cannot be pushing. On the other hand, when the rear locomotive pushes the train, the buffers press hard against each other, which makes the coupling become slack, thus rendering the front locomotive useless. It turns out that the locomotives cannot be moving the train at the same time since only one of them is working at a time. Why then do they employ two locomotives? The Speed of a Train You are travelling in a train and want to find its speed, could you work it out from the clatter of the wheels? Two Trains Two trains once left their respective stations for the other’s station simultaneously. The first arrived at its destination an hour after the two trains had met each other. The second reached its destination 2 hours 15 minutes after the same event. How many times faster was the first train? The problem can be done using mental arithmetic. How Does a Train Start From Rest? You may have noticed that before making a train move forward the engine-driver sometimes makes it push back. Explain why. Problems on Transport A Race Two sailing boats are competing against each other. They must sail 24 kilometres there and back in the shortest time possible. The first boat covered the whole route with a uniform speed of 20 kilometres an hour whilst the second boat sailed the outward leg at 16 kilometres an hour and sailed back at 24 kilometres an hour. The first boat won, though it would seem that the second one should have gained during the return trip exactly what it lost out during the first section of the route. It should thus have come in at the same time as the first boat. Why did it lag behind? Steaming Up and Down the River A steamer makes 20 kilometres an hour downstream and 15 kilometres an hour upstream. A trip between two towns takes it 5 hours less than the return trip. What is the distance between the towns? Answers 212-213 m f ^ O A Plane's Flight There is actually nothing to explain here, the aircraft takes the same time to travel in both directions. The problem has a catch for the inattentive reader who might think that 1 hour 20 minutes and 80 minutes are different times. Strange as it might seem, many people swallow this bait, and people used to adding up are more likely to make it than those who aren’t The explanation lies in the habit of dealing with metric system of measures and money. We are apt to treat “1 hour 20 minutes” and “80 minutes” just like “1 pound 20 pence” and “80 pence”, say, or “1 dollar 20 cents” and “80 cents”. So it’s really a psychological problem. Two Locomotives The way it works out is as follows. The front locomotive does not take care of the whole of the train, but only part of it, about half the carriages. The rest of them are pushed by the rear locomotive. The couplings between the first group of carriages are taut whilst they are slack between the rear ones which are being pushed buffer to buffer. The Speed of a Train You must have noticed that when travellingin a train you feel regular jerks all the time which the springs, however good, cannot suppress. These jerks come from the wheels being slightly jarred at rail junctions (Fig. 215) and are transferred throughout the carriage. Figure 215 This nuisance, which is also bad both for the carriages and the tracks, lends itself for measuring the speed of the train. You only need to count the number of jerks you feel in one minute to find how many rails you’ve passed. Now you only have to multiply this number by the length of a rail to arrive at the distance covered by the train during that minute. The regulation length of a rail is about 15 metres*. So, multiply the number of jerks a minute by 15 and then by 60, divide the result by 1,000 and you’ll obtain the * You may work out the length of a rail by pacing it out, seven paces amounting to about 5 metres. Answers number of kilometres covered by the train per hour. So, (number of jerks) x 15 x 60 UXX) = kilometres per hour. Two Trains The faster train arrives at the meeting point having covered a distance that is larger than the distance covered by the slower train by as many times as the speed of the faster train is higher than that of the slower train. After the meeting each train has to pass the distance that had been covered by the other one. In other words, the faster train covered a distance after the meeting that was as many times shorter than the distance covered by the slower train as its speed was higher. If we denote the ratio of the two speeds by x, then the faster train took x2 times less time than the other to cover the distance from the meeting point to the respective station. Hence x2 = 2 1/4 and x = 1 1/2, i.e. the first train is 1.5 faster than the second train. How Does a Train Start From Rest? When a train arrives at a station and comes to rest, the couplings between the carriages are taut. If the locomotive is to begin to pull the train like this, it would have to start the whole of the train from rest at once, which might be too difficult a task for it. On the other hand, if the locomotive first pushes the train backwards the couplings are no longer taut and the train is started from rest carriage by carriage in succession and that is much easier. In other words, the engine-driver does what a coachman does sometimes when the coach is heavily loaded, i.e. he starts the coach and only then jumps on it, otherwise the horse would have to push more load from rest. A Race The second boat lagged behind because it travelled at 24 kilometres an hour for a shorter time than it travelled at 16 kilometres an hour. In fact, it travelled at 24 km/h for 24/24 hours, i.e. 1 hour, and at 16 km/h for 24/16 hours, i.e. 1 1/2 hours. Therefore, it lost more time on the journey “there” than gained on the way “back”. Steaming Up and Down the River Travelling downstream the steamer covers 1 kilometre in 3 minutes whilst travelling upstream it covers 1 kilometre in 4 minutes. In the first case, the steamer gains 1 minute every kilometre, and as the total gain is 5 hours, or 300 minutes, the distance between the towns is 300 kilometres. Really, 300 300 214-215 Surprising Calculations A Glass of Peas Of course, you’ve seen peas many times and held a glass in your hand, so that you must know the sizes of these things. Imagine a glass filled to the brim with dry peas. Thread all the peas on a piece of string like beads. If the string is stretched, how long would it be approximately? Water and Wine One bottle contains a litre of wine, another a litre of water. A spoonful of wine is transferred from the first bottle into the second, and then a spoonful of the mixture thus obtained is transferred from the second bottle into the first one. What do we now have, more water in the first bottle or more wine in the second? Figure 216 A Die Figure 216 shows a die, i.e. a cube with from 1 to 6 points on its six faces. Peter bets that if the cube is thrown four times in succession, then it is bound to show 1 at least once. But Vladimir argues that the 1 will either not appear at all with the four throws or it will show more than once. Who stands the better chance of winning? The Yale Lock The Yale lock was invented by an American, Linus Yale, Jr., in 1865, and has come to be almost universally used ever since. Despite its long history, some people question the possibility of having a large number of versions of the lock. But we need only to look at the construction of the lock to see that it provides for an almost unlimited number of variations. Figure 217 depicts the front view of the Yale lock. You see a small circle around the key hole which is the end face of the cylinder passing through the depth of the lock. The lock opens when the cylinder turns, but this is the crunch. The cylinder is secured by five short Surprising Calculations 9 * • Figure 217 Figure 218 steel pins (Fig. 217, right). Each pin actually consists of two pins, and the cylinder can only be turned when the double pins are so arranged that the cut lie at the boundary of the cylinder. The pins are arranged this way using a key with serrated edge. You just insert the key into the keyhole and the pins are lifted to the height required for the lock to open. You can easily see now that the number of the various combinations of heights in the lock can be exceedingly large. It depends on the number of ways in which each pin may be severed. Suppose that each pin may be divided into two parts in 10 ways only. Try and work out the number of combinations possible for the Yale lock. How Many Portraits? Draw a portrait on a sheet of cardboard and cut it into several-say nine-stripes. Next draw other stripes showing various parts of the face so that any two neighbouring stripes belonging to different portraits might be fitted into another portrait without interrupting the lines. If you prepare, say, four stripes * for each part of the face, you’ll have 36 stripes all in all. * These could be conveniently glued onto four faces of a square block. 216-217 Surprising Calculations You’ll now be able to make up a variety of faces by taking nine stripes each time. Shops once used to sell ready-made sets of these stripes (or blocks) to make up portraits (Fig. 218). It was claimed that of 36 stripes one could produce a thousand various faces. Is it so? Abacus Perhaps you can use the abacus and can set, say, 25 pounds, on it. But the problem becomes more difficult if you must shift not seven beads, as usual, but 25 beads. Just try. To be sure, nobody is going to do so in practice, but the problem is not intractable and the answer is rather curious. Leaves of a Tree If we were to take all the leaves from an old tree, say a lime-tree, and place them side by side without any breaks, how long approximately would the line be? Would it be possible, for example, to encircle a large house with it? A Million Steps You must know what a million is and can estimate the length of your step, so that you should easily be able to say how far would a million steps take you? More than 10 kilometres away? Or less? Cubic Metre A teacher asked his class if they were to put all the millimetre cubes contained in cubic metre, on top of each other, how high would the column be? “It’d be higher than the Eiffel Tower (300 metres)!” one student exclaimed. “Even higher than Mont Blanc (5 kilometres)!” another answered. Which was closer to the truth? Whose Count Was Higher? Two people kept count of the passers-by on a pavement over a period of an hour. One of them stood near the gate of a house whilst the other strolled to and fro along the pavement. Whose count was higher? Answers 9 ® A Glass of Peas Any guess here will lead you to an error. A calculation, however crude, is in order. A dry pea is about 1/2 centimetreacross. A centimetre cube contains no less than 2 x 2 x 2 = 8 peas (if tightly packed, even more). In a glass of capacity 250 cubic centimetres there are no less than 8 x 250 = 2,000 peas. When strung these would give a line 1/2 x 2,000 = 1,000 centimetres long, i.e. 10 metres. Water and Wine In solving the problem we mustn’t overlook the fact that the final volume of liquid in the bottles was equal to the initial one, 1 litre. We then argue as follows. Let, after both transferrals, the second bottle contain n cubic centimetres of wine, and hence (1,000 — n) cubic centimetres of water. Where have the missing n cubic centimetres of water gone? Clearly, these are to be found in the first bottle. Accordingly, the wine in the end contains as much water as there is wine in the water. A Die The number of all the possible events after four throws of the die is 6 x 6 x 6 x 6 = = 1,296. Suppose that the die has already been thrown once and a 1 appeared. Then for the three remaining throws the number of all the possible events, favourable for Peter, i.e. the occurrence of any face save for the 1, will be 5 x 5 x 5 = 125. In exactly the same way, 125 outcomes favourable for Peter are possible if the 1 appears only in the second, only in the third or only in the fourth throw. So, there are 125 + 25 + + 125 + 125 = 500 various possibilities for the 1 to appear once, and only once, in the four throws. As to the unfavourable outcomes, there are 1,296 — 500 = 796 since all the remaining events are unfavourable. Thus, we see that Vladimir stands better chance to win than Peter: 797 against 500. The Yale Lock It’s easily seen that the number of different locks possible is lOx lOx lOx lOx 10 = = 100,000. Each of these locks can only be opened by their own key. It is very comforting for the owner of the lock that there are 100,000 versions of the lock and key as the lock picker has only one chance in 100,000 to hit upon the right key. Our calculation is very rough since it assumes that each pin can only be divided in 10 different ways. Clearly it could actually be done in a larger number of ways, thus notably increasing the number of different locks possible. This shows the advantage of the Yale lock. How Many Portraits? Far more than a thousand. To show this is true make each of the nine sections of a portrait with one of the Roman numerals I, II, III, IV, V, VI, VII, VIII and IX. For Answers 218-219 each section there are four stripes, so we’ll mark these by 1, 2, 3 and 4. Take stripe 1.1. It may go to II. 1, II.2, II.3, or II.4, i.e. we may have four combinations. But since section I may be represented by four stripes (1.1, 1.2, 1.3, or 1.4) each of which may be connected to II in four ways, then the two upper sections I and II may be joined in 4 x 4 = 16 various ways. To each of these 16 arrangements we may attach section III in four ways (III.1, III.2, III.3, or III.4). Consequently, the first three sections may be combined in 16 x x 4 = 64 various ways. Reasoning along the same lines, we find that I, II, III, and IV may be arranged in 64 x 4 = 256 various ways: I, II, III, IV, and V, in 1,024 ways: I, II, III, IV, V, and VI, in 4,096 ways, and so forth. Lastly, all the nine sections may be fitted together in 4 x x4x4x4x4x4x4x4x4 = 262,144 ways. Not one thousand but more than a quarter of a million different portraits! The problem is a very instructive one and it goes to explain why it’s only exceptionally rarely that we may come across two similar faces. We’ve just seen that if the human face were characterized by as few as nine features with only four versions possible, then it would be more than 260,000 various faces in existence. In actuality, there are more than nine features and they may vary in more than four ways. In fact, if there were 20 features varying in 10 ways each, we would have 1020, or 100,000,000,000,000,000,000, ways. Incidentally, this is many times greater than the world’s population. Abacus You can set 25 pounds using 25 beads in the following way: Figure 219 Actually, this gives 20 pounds + 4 pounds + 90 pence + 10 pence = 25 pounds. The number of beads is 2 + 4 + 9 + 10 = 25. Leaves of a Tree A small town, let alone a house, could be encircled with the leaves from a tree if we arranged them in a line because the line would be about 12 kilometres long! Really, the foilage of mature tree includes no less than 200-300 thousand leaves. If for definiteness we stick to 250 thousand and take a leaf to be 5 centimetres wide, we’ll have a line 1,250,000 centimetres long, which is 12,500 metres, or 12.5 kilometres. Answers 9 ® A Million Paces A million paces is much more than 10 or even 100 kilometres. If an average pace is about 3/4 metre long, then 1,000,000 paces = 750 kilometres. Since the distance from Moscow to Leningrad is about 640 kilometres, then a million paces would take farther than Leningrad. A Cubic Metre Both answers are far from the true figure because the column would be 100 times higher than the highest mountain on Earth. Indeed, in a cubic metre there are 1,000 x x 1,000 x 1,000 = 1 milliard cubic millimetres. If you put one on top of another they would form a column 1,000,000,000 millimetres high or 1,000,000 metres, or 1,000 kilometres. Whose Count Was Higher? The counts were equal. Predicaments Instructor and Student The story related below is said to have occurred in Ancient Greece. The teacher and thinker Protagoras (485-410 B. C.) undertook to teach a young man the art of being a barrister. The two sides made a deal that the student pay the fee just after he had made some achievement, i. e. after he had won his first trial. The student passed the course and Protagoras was waiting for his reward, but the student wouldn’t appear in a court of justice. What was to be done? To get his fee the teacher sued his student. He argued thus: if he won the case, the money would be recovered by the court, whereas if he lost the case, and hence his student won it, the money would again be paid according to their deal. The student, however, regarded Protagoras’s case as absolutely hopeless (he seems to have learned something from his teacher) and reasoned as follows: if the judge decided against him, he wouldn’t pay according to the terms of the deal since he would have lost his first case, whereas if the judge decided in his favour, again he wouldn’t have to pay since that would be the decision of the court. The judge was embarrased but after a great deal of thought he hit upon an idea and passed a decision that, without violating the terms of the deal, gave the teacher an opportunity to recover his fee. What was the decision? The Legacy Here is another ancient problem that was a favourite with lawyers in Ancient Rome. A widow has to share a legacy of 3,500 sestertii with her child who was about to be bom. According to Roman law, if the child were a boy, his mother got a half of the son’s share but if it were a girl, the mother got double the share of the daughter. But it so happened that twins were bom, a boy an a girl. How was the legacy to be shared so that the law was completely satisfied? Pouring Consider of jug containing 4 litres of milk. The milk must be divided equally between two friends, but the Predicaments only containers available are two empty jugs, one of which holds 2 1/2 litres and the other holds 1 1 /2 litres. How can the milk be divided using the three jugs? Of course, it’ll be necessary to pour the milk from one jug into another. But how? Two Candles The electricity failed in my flat because the fuse had blown. I lighted two candles that had been specially prepared on my desk, and worked on in their light until the failure was set right. The next day they wanted to know how long the electricity was off. I had not noticed the time when the electricity failed and was restored,and I didn’t know the initial length of the candles. I only knew that the candles were the same length but different thicknesses, and that the thicker one took 5 hours to burn down completely whilst the thinner one took 4 hours. Both were new before I had lighted them up. But I didn’t find the ends of the candles: somebody had thrown them away. I was told that the stubs were so small that it wouldn’t have paid to keep them. “But couldn’t you remember their lengths?” I asked. “They weren’t the same. One was four times longer than the other”. All my attempts to squeeze out something more failed. I had to be content with the above information and try to work out how long the candles had been burning. How would you handle the problem? Three Soldiers Three soldiers were having a problem, too. They had to cross a river without a bridge. Two boys with a boat agreed to help the soldiers but the boat was so small it could only support one soldier and even then a soldier and a boy couldn’t be in the boat for fear of sinking it. None of the soldiers could swim. It would seem that under these conditions only one soldier could cross the river. However, all three soldiers were soon on the other bank and returned the boat to the boys. How did they do it? 222-223 Predicaments A Herd of Cows Here is one of the versions of a curious ancient problem. A father distributed his herd amongst his sons. To his eldest he gave one cow plus 1/7 of the remaining cows; to his second eldest, two cows plus 1/7 of the remaining cows; to the third eldest, three cows plus 1/7 of the remaining cows; to the fourth eldest, four cows and 1/7 of the remaining cows, and so forth. The herd was distributed among his sons without remainder. How many sons and how many cows were there? Square Metre When a boy was told for the first time that a square metre contains a million square millimetres, he wouldn’t believe it. “Why so many?” he was surprised. “Here I’ve got a sheet of graph paper that is exactly one metre long and one metre wide. And are there million millimetre squares here? I don’t believe it!” “Count them then,” somebody advised. The boy decided to do so and count all the squares. He got up early in the morning and set about counting them neatly marking each square he had counted with a point. Each mark took him a second so the going was rather fast. He worked like blazes, still do you think he managed to make sure that a square metre has a million square millimetres on the same day? A Hundred Nuts A hundred nuts are to be divided between 25 people so that nobody gets an even number of nuts. Could you do it? Dividing Money Two people were making porridge on a camp-fire. One contributed 200 grammes of cereals, the other 300 grammes. When the porridge was ready, they were joined by a passer-by who partook of their meal and paid them 50 pence. How should they divide the money? Predicaments Sharing Apples Nine apples must be shared out amongst 12 children so that no apple is divided into more than four parts. On the face of it the problem is insolvable, but those who knows about fractions can solve it easily. Once you have solved that one it should be easy to handle another problem in the same vein: to divide seven apples among 12 boys so that none of the apples is divided into more than four parts. A Further Apple Problem Five friends came to see Peter. Peter’s father wanted to treat all six boys to apples but there were only five apples. What was to be done? Everyone had to have his fair share. The apples, of course, had to be cut but not into small pieces since Peter’s father wouldn’t cut them into more than three. So, the problem was to divide the five apples equally among the six boys so that none of the apples was cut into more than three pieces. How was Peter’s father to get out of his predicament? One Boat for Three Three sports enthusiasts possess one boat. They keep it on a chain with three locks so that each of them could use it but a stranger couldn’t. Each of them has his own key but he can still unlock the boat without waiting for his friends and their keys. How did they arrange it? Waiting for a Tram Three brothers came to a tram stop. There was no tram in sight and the eldest brother suggested they wait. “Why wait?” the second brother asked, “we’d better go on. When the tram catches up with us, we can jump onto it, but by then we’d have got part of the way home and thus we’ll get there sooner.” “If we decide to go,” the youngest brother objected, “then we’d better go backwards not forwards: since then we’ll meet an oncoming tram sooner and so get home sooner.” Since the brothers couldn’t persuade each other, each went his own way. The eldest stayed to wait, the second went on, and the youngest walked back down the route. Which of the three got home sooner? Who was the most reasonable? 224-225 Answers ?5 Q») Instructor and Student The decision was to decide against Protagoras but give him the right to bring the case before the court a second time. After the student had won his first trial, the second one should undoubtedly be decided in favour of the instructor. The Legacy The widow gets 1,000 sestertii, the son 2,000 sestertii, and the daughter 500 sestertii. This fulfils Roman law since the widow gets a half of the son’s share and double the daughter’s. Pouring Seven pourings will be required as is shown in the table: Pouring 41 11/21 21/21 1 1 1/2 _ 2 1/2 2 1 1/2 1 1/2 1 3 3 — 1 4 3 1 — 5 1/2 1 2 1/2 6 1/2 1 1/2 2 7 2 — 2 Two Candles We’ll construct a simple equation. We’ll denote the time (in hours) that the candles burned by x. Each hour 1/5 part of the original length of the thick candle and 1/4 part of the original length of the thin candle bums away. Accordingly, the thick candle’s stub will be 1 — x/5 of its original length and the thin candle’s stub 1 — x/4 of the original length. We know that the candles were originally equally long and that the four times the length of the thick stub, i.e. 4(1 — x/5), was equal to the length of the thin stub (1 — x/4). Thus, 4 = 1 - x T' Solving the equation gives that x = 3 3/4 hours, i. e. the candles had burned for 3 hours 45 minutes. Three Soldiers The following six crossings were made: 1st crossing. Both boys go to the opposite bank and one of them brings the boat back to the soldiers (the other stays on the opposite bank). 15-621 Answers '5 © 2nd crossing. The boy that brought the boat back stays on the bank with the soldiers and a soldier crosses the river in the boat. The boat returns with the other boy. 3d crossing. Both boys cross the river and one of them returns with the boat. 4th crossing. The second soldier crosses and the boat returns with the boy. 5th crossing. Like the third one. 6th crossing. The third soldier crosses and the boat returns with the boy. The boys continue on their journey and the three soldiers are on the opposite bank. A Herd of Cows Arithmetically (i. e. without resorting to equations), the problem should be approached from the end. The youngest son got as many cows as there were sons for he could not get an additional 1/7 of the remaining herd as there were no cows left. Further, the next son got one cow less than there were sons, plus 1/7 of the remaining cows. Accordingly, the share of the youngest son amounts to 6/7 of the share of the remainder. It thus follows that the number of cows the youngest son got must be divisible by six. Let’s assume that the youngest son received six cows and see if this assumption is good. It follows from the assumption that there were six sons. The fifth son got five cows plus 1/7 of seven, i.e. six cows all in all. Thus, the two youngest sons got 6 + + 6=12 cows, which accounts for 6/7 part of the herd left after the fourth son has received his share. The totalresidue was 12+6/7 = 14 cows, hence the fourth son got 4 + 14/7 = 6 cows. We’ll now work out the residue after the third son got his share: 6 + 6 + 6= 18 cows is 6/7 part of the residue. Therefore, the total residue was 18—+6/7 = 21 cows. The third son got 3 + 21/7 = 6 cows. In exactly the same way we’ll find that the second and first sons also got six cows each. Our assumption that there were six sons and 36 cows appears to be plausible. But are there other solutions? Assume that there were 12 sons, not six. It turns out that this assumption is unsuitable. The number 18 won’t do either. Other multiples of six would be unreasonable since there couldn’t be 24 or more sons. Square Metre No, the boy would not be able to verify the fact in one day. Even if he counted for 24 hours without interruption, he would have counted only 86,400 squares since there are only 86,400 seconds in 24 hours. To count to one million he would have to work for almost 12 days without stopping, and for a month if he worked 8 hours a day. + Hundred Nuts Many people would immediately set about trying a variety of combinations, but their efforts would all be to no avail. If you give some thought to the problem, you’ll understand the futility of all their efforts since the problem is insolvable. Answers 226-227 If you could break 100 into 25 odd summands, you would have been able to make an odd number of odd numbers add up to 100 which is an even number, and that is clearly impossible. In fact, we would have to obtain 12 pairs of odd numbers and one more odd number. Each pair of odd numbers yields an even number, so 12 pairs of even numbers must add up to an even number. If then we add an odd number to the total, we’ll end up with an odd result. Thus 100 can never be composed of such summands. Dividing Money Most people answer that the one who contributed the 200 grammes should get 20 pence and the other 30 pence. This division is not fair. We’ll argue as follows: 50 pence was paid for one portion of food. Since there were three eaters, the cost of the porridge (500 grammes) should be 1 pound 50 pence. The person who contributed the 200 grammes gave 60 pence worth of food in terms of money (since a hundred grammes costs 150-+5 = 30 pence). However, he also consumed 50 pence worth of porridge, hence he must get back 60 — — 50 = 10 pence. The contributor of the 300 grammes (i.e. 90 pence in terms of money) must get 90 — 50 = 40 pence. Thus, out of the 50 pence one person should have 10 pence and the other person 40 pence. Sharing Apples It’s possible to share nine apples equally between 12 children without cutting any apple into more than four parts. Six apples should be divided in two each to yield 12 halves. The remaining three apples should each be divided into four equal parts to yield 12 quarters. Now each child receives a half and a quarter. So each will get 3/4 of an apple as required, because 9-+12 = 3/4. Reasoning along the same lines it’s possible to divide seven apples among 12 children so that each child gets an equal share and no apple needs to be cut into more than four parts. In this case each child should get 7/12 of an apple, but notice that 7/12 = 3/12 + 4/12= 1/4+ 1/3. Therefore three apples are divided into four parts and the four remaining apples into three parts each. We thus obtain 12 quarters and 12 thirds. In consequence, each child can be given a quarter and a third, or 7/12. + Further Apple Problem The apples were divided thus: three apples were each cut in half to yield six halves that were distributed among the children and the remaining two apples were each cut into three to obtain six thirds that were also given to the children. Consequently, each boy got a half and a third of an apple, i. e. all the boys got their equal share, and none of the apples was cut into more than three equal parts. 15* Answers ’5 CD One Boat for Three The locks should be connected as shown in Fig. 220. You can see quite easily that each of the boat’s owners can open the chain of the three locks using his key. Figure 220 Waiting for a Tram The youngest brother, who went backwards, saw an oncoming tram and jumped into it. When the tram came to the stop where the eldest brother was waiting, he got in too. A short while later the tram caught up the third brother who was walking homewards and collected him. All the three brothers found themselves in the same tram and, of course, arrived home at the same time. The most reasonable brother was the eldest one since he waited quietly at the stop. Problems from Gulliver's Travels Beyond doubt the most fascinating pages in Gulliver’s Travels are those describing his unusual adventures in the country of tiny Lilliputians and in the country of giant Brobdingnagians. In Lilliput the dimensions - height, width, thickness-of people, animals, plants and other things were 1/12 of those here. By contrast, in Brobdingnag they were 12 times larger. We can easily understand why the author of the Travels choose the number 12, if we remember that in the British system of units there are 12 inches in a foot. A 12-fold increase or decrease doesn’t seem to be very much of a change but the nature and way of life in this fantastic countries was strikingly different from those we are used to. Every now and then the differences are so amazing that can serve as a material for interesting problems. Animals of Lilliput Gulliver relates: “Fifteen hundred of the Emperor’s largest horses... were employed to draw me towards the metropolis.” Doesn’t it seem to you that 1,500 horses are a bit too many taking into account the relative dimensions of Gulliver and Lilliputian horses? Also, Gulliver tells us a no less amazing thing about the cows, bulls, and sheep, for when he left he just “put them into his pocket”. Is it all possible? Hard Bed Lilliputians made the following bed for their giant guest: “Six hundred beds of the common measure were brought in carriages, and worked up in my house; a hundred and fifty of their beds sewn together made up the breadth and length, and these were four double, which however kept me but very indifferently from the hardness of the floor, that was of smooth stone”. Why was Gulliver so incomfortable on the bed? And is this computation correct? Gulliver’s Boat Gulliver left Lilliput in a boat washed up on the shore by chance. The boat seemed monstrous to the Problems from Gullivers Travels Lilliputians, it surpassed by far the largest ships of their fleet. Could you work out the displacement* of the boat in Lilliputian tonnes if its weight-carrying capacity was 300 kilogrammes? Hogsheads and Buckets of Lilliputians Gulliver is drinking: “I made another sign that I wanted drink... They slung up with great dexterity one of their largest hogsheads; then rolled it towards my hand, and beat out the top; I drank it off at a draught, which I might well do, for it hardly held half a pint... They brought me a second hogshead, which I drank in the same manner, and made signs for more, but they had none to give to me”. Elsewhere in the book Gulliver describes the Lilliputian buckets as being no larger than a thimble. Why should such tiny hogsheads and buckets exist in a country where everything is only 1/12th normal size? Food Allowance and Dinner Lilliputians set the following daily allowance of food for Gulliver: "... the said Man Mountain shall have a daily allowance of meat and drink, sufficient for the support of 1,728 of our subjects.” Elsewhere Gulliver relates: “I had three hundred cooks to dress my victuals, in little convenient huts built about my house, where they and their families lived, and prepared me two dishes apiece. I took up twenty waiters in my hand, and placed them on the table; a hundred more attended below on the ground, some with dishes of meat, and some withbarrels of wine and other liquors slung on their shoulders; all which the waiters above drew up as I wanted, in a very ingenious manner, by certain cords, as we draw the bucket up a well in Europe”. How did they come to fix on that number? And what is the use of all that army of servants to feed just one man? After all, he’s only a dozen times taller than a Lilliputian. Are the allowance and appetites compatible with the relative sizes of Gulliver and the Lilliputians? * The displacement of a ship is the largest load (including the weight of the ship itself) that the ship can support. 230-231 Problems from Gulliver's Travels Figure 223 Three Hundred Tailors “Three hundred tailors were employed... to make me clothes.” Was this army of tailors really necessary to have clothes made for a man who is only a dozen times larger than a Lilliputian? Gigantic Apples and Nuts In the part “A Voyage to Brobdingnag” devoted to Gulliver’s stay in the country of giants we read about some of the hero’s trouble-filled adventures. So once he was in the gardens of the court under some apple-trees and the Queen dwarf “when I was walking under one of them, shook it directly over my head, by which a dozen apples, each of them near as large as a Bristol barrel, came tumbling about my ears; one of them hit me on the back as I chanced to stoop, and knocked me down flat on my face.” On another occasion “an unlucky schoolboy aimed a hazelnut directly at my head, which very narrowly missed me; otherwise, it came with so much violence, that it would have infallibly knocked out my brains; for it was almost as large as a small pumpkin”. What do you think was the weight of the apples and nuts in Brobdingnag? A Ring of the Giants The collection of rarities brought by Gulliver from Brobdingnag includes “a gold ring which one day she (the Queen) made me a present of in a most obliging manner, taking it from her little finger, and throwing it over my head like a collar.” Is it possible that a ring from a little finger would fit on Gulliver like a collar and how much, approximately, would the ring weigh? Books of the Giants About books of Brobdingnagians Gulliver tells us the following: “I had liberty to borrow what books I pleased. The Queen’s joiner had contrived... a kind of wooden machine five and twenty foot high, formed like a standing ladder; the steps were each fifty foot long. It was indeed a movable pair of stairs, the lowest end placed at ten foot distance from the wall of the Problems from Culliver's Travels chamber. The book I had a mind to read was put up leaning against the wall. I first mounted to the upper step of the ladder, and turning my face towards the book, began at the top of the page, and so walking to the right and left about eight or ten paces according to the length of the lines, till I had gotten a little below the level of my eye; and then descending gradually till I came to the bottom; after which I mounted again, and began the other page on the same manner, and so turned over the leaf, which I could easily do with both my hands, for it was as thick and stiff as a pasteboard, and in the largest folios not above eighteen or twenty foot long.” Does this make sense? Collars for the Giants Finally, consider a problem of this kind that is not directly taken from Gulliver's Travels. You may know that the size of a collar is nothing but the number of centimetres of its length. If your neck is 38 centimetres round, your collar size is 38. On average an adult’s neck is 40 centimetres round. If Gulliver wished to order some collars in London for a Brobdingnagian, what number would he require? 232-233 Answers 16 Animals of Lilliput It’s calculated in the answer to “Food Allowance and Dinner” that Gulliver’s volume was 1,728 times larger than that of a Lilliputian. Crearly, he was that many times heavier. For Lilliputians it was as difficult to transport his body as it would have been to transport 1,728 grown-up Lilliputians. That is why the cart with Gulliver had to be pulled by so many Lilliputian horses. Animals in Lilliput were also 1,728 times smaller in volume, and hence as much lighter than ours. Our cow is about 1.5 metres high and weighs 400 kilogrammes. A cow in Lilliput would be 12 centimetres high and weigh 400/1,728 kilogrammes, i.e. less than 1/4 kilogrammes. A toy cow like this really could be carried about in a pocket. Gulliver gives a true account of relative sizes: “The tallest horses and oxen are between four and five inches in height, the sheep an inch and a half, more or less; their geese about the bigness of a sparrow, and so the several gradations downwards, till you come to the smallest, which to my sight were almost invisible... I have been much pleased with observing a cook pulling a lark, which was not so large as a common fly; and a young girl threading an invisible needle with invisible silk.” Hard Bed The calculation is quite correct. If a Lilliputian bed is 12 times shorter, and of course 12 times narrower than a conventional bed, then its surface area would be 12 x 12 times smaller than the surface of our bed. Accordingly, for his bed Gulliver required 144 (i.e. to make a round number, about 150) Lilliputian beds. The bed would however have been exceedingly thin-12 times thinner than ours. Thus even four layers of such beds would not have been soft enough for Gulliver since the resultant mattress was three times thinner than ours. Answers 16 © Gulliver's Boat We know from the question that the boat could carry 300 kilogrammes, i. e. its displacement was about 1/3 tonne. A tonne is the weight of 1 cubic metre of water, hence the boat displaced 1/3 of our cubic metre. But all the linear dimensions in Lilliput are 1/12 of ours, and volumes are 1/1,728 of ours. So 1/3 of our cubic metre contains about 575 Lilliputian cubic metres and thus Gulliver’s boat had a displacement of 575 tonnes or thereabout since we arbitrarily took the figure 300 kilogrammes. Today we have ships with displacements of tens of thousands of tonnes ploughing the seas, so a ship with a 575-tonne displacement should not be a wonder. We should remember though that at the time of writing (early in the 18th century) 500-600-tonne ships were still rare. Hogsheads and Buckets of Lilliputians Lilliputian vessels were 12 times smaller than ours in every dimensions-height, width, and length-and 1,728 times smaller in volume. If we assume that our bucket contains about 60 glasses, we can work out that a Lilliputian bucket contains only 60/1,728, i.e. about 1/30 of a glass. This is just larger than a tea-spoonful but not really much larger than the volume of a large thimble. If the capacity of a Lilliputian bucket is thus a tea-spoonful, the capacity of a 10-bucket hogshead would not be much larger than half a glass. No wonder Gulliver couldn’t quench his thirst with two such hogsheads. Food Allowance and Dinner The computation is perfectly correct. We shouldn’t forget that Lilliputians were an exact, though smaller, replica of conventional people with normally proportioned members. Consequently, they were not only 12 times shorter, but also 12 times narrower and 12 times thinner than Gulliver, and their volume was 1/1,728 of that of Gulliver. And to support the life of such a body requires respectively more food. That’s why Lilliputians calculated that Gulliver needed an allowance sufficient to support 1,728 Lilliputians. We now see the purpose of so many cooks. To make 1,728 dinners requires no less than 300 cooks taking that one Lilliputian cook can make half a dozen Lilliputian dinners. An accordingly larger number of people is required to haul the load up to Gulliver’s table, which can be estimated to be the height of a three-storey building in Lilliput. Three Hundred Tailors The surface of Gulliver’s body was 12x12, i.e. 144 timeslarger than that of a Lilliputian. This is clearer if we imagine that each square inch of the surface of a Lilliputian’s body corresponds to a square foot on the surface of Gulliver’s body. We know, however, that there are 144 square inches in a square foot. Thus Gulliver’s suit would take 144 times more fabric than that of a Lilliputian, and hence more Answers 234-235 working time. If, say, one tailor can make one suit in two days, then to make 144 suits in a day (or one of Gulliver’s suits) may require 300 tailors. Gigantic Apples and Nuts An apple that weighs about 100 grammes here should correspond to an apple in Brobdmgnag that is as many times heavier as it is bigger in volume, i.e. 1,728 times heavier than here. Thus Brobdingnagian apples are about 173 kilogrammes. If such an apple falls from a tree and hits a man on the back, he would only just survive the blow. Gulliver thus got off lightly. Figure 225 A Brobdingnagian nut must have weighed 3-4 kilogrammes, if we take that our nut weighs about 2 grammes. Such a gigantic nut might be about a dozen centimetres across. A 3-kilogramme, hard object thrown with the speed of the nut clearly could smash the skull of a normal-size man. Elsewhere in the book Gulliver recalls: “There suddenly fell such a violent shower of hail, that I was immediately by the force of it struck to the ground: and when I was down, the hailstones gave me such cruel bangs all over the body, as if I had been pelted with tennis balls.” Quite plausible, because each piece of hail in this country of giants must weigh no less than a kilogramme. A Ring of the Giants A normal little finger is about 11/2 centimetres across. Multiplying this by 12 gives 18 centimetres and a ring of such a diameter has a circumference of 56 centimetres, i. e. Figure 226 Answers it’s sufficiently large for a normal head to go through it. As to the weight of such a ring, if a normal ring weighs 5 grammes its counterpart in Brobdingnag must have weighed 8 1/2 kilogrammes! Books of the Giants If we start from the size of books current in our times (about 25 centimetres long and 12 centimetres wide), then Gulliver’s account might appear to be a slight exaggeration. Figure 221 You could handle a book 3 metres high and 1 1/2 metres wide without a ladder and without having to move to the left or right by 8-10 steps. In the days of Swift, early in the 18th century, the conventional format of books (tomes) was far larger than now. 20 x 30 cm formats were not uncommon, which when multiplied by 12 gives 360 x x 240 centimetres. It is impossible to read a 4-metre book without a ladder. But a real tome of the time might be as large as a newspaper. However, the modest tome we mentioned would in the country of giants weigh 1,728 times more than here, i.e. about 3 tonnes. Assuming that it has 500 sheets, each of its sheets would weigh about 6 kilogrammes, perhaps a bit too much for fingers. Collars for the Giants The neck of a giant will be 12 times larger than that of a normal man. And if a normal man needs a collar of size 40, the giant would need a 40 x 12 = 480 size collar. * * * We thus see that all the whimsical things in Swift seem to have been carefully calculated. Responding to certain critisisms of his poem Eugine Onegin Alexander Pushkin once noted that in his book “time is calculated with a calendar”. In exactly the same way Swift could say that all his objects had conscientiously been computed using the laws of geometry. Stories about Giant Numbers Reward According to legend, the following happened in ancient Rome. I. General Terentius had returned to Rome with booty after a victorious campaign. Back in the capital he was received by the Emperor. The reception was very warm and the Emperor thanked him cordially for his services to the Empire promising to confer on him a high office in the Senate. But Terentius didn’t want this. He said: “I have won many victories to exalt your grandeur. Sire, and to cover your name with glory. I have been unafraid of death and if I had many lives. I’d sacrifice all of them to you. But I’m tired of fighting, my youth had passed and my blood flows slower in my veins. The time has come for me to retire to my father’s home and revel in the joys of domestic life.” “What would you like to receive from me, Terentius?” the Emperor asked. “Hear me out with indulgence, Sire! In all these long years of battle, imbruing my sword with blood, I have had no time to take care of my well-being. I’m poor. Sire...” “Proceed, brave Terentius.” The encouraged general went on to say: “If it is your desire to reward your humble servant, then may your generosity help me live out the remainder of my days in peace and comfort at home. I do not seek honour or high office as I would like to retire from power and public life to live peacefully. Sire, please award me with money to provide for the rest of my life.” The Emperor-so the legend goes-wasn’t distingui¬ shed for his lavishness. He liked to save money for him¬ self but was miserly with it to others. The general’s request plunged him in a deep reverie. He asked, “What sum, Terentius, would you consider sufficient?” “A million denarii. Sire.” The Emperor grew pensive again. The general waited, his head down. Finally, the Emperor spoke: “Valiant Terentius, you are a great warrior and your prodigies of valour have earned you a lavish reward! I will give you wealth. Tomorrow at noon you will hear Stories about Giant Numbers my decision.” Terentius bowed and walked out. Figure 228 II. On next day at the hour appointed the general came to the Emperor’s palace. “Greetings, brave Terentius!” the Emperor said. Terentius bowed his head humbly. “Sire, I came to hear your decision. You kindly promised to reward me.” The Emperor answered: “It’s not my intention that such a noble warrior like you should have some miserable reward for his heroic deeds. Listen to me. There are in my treasury 5 million copper brasses*. You shall go to the treasury and take one coin, then you shall return here and place it at my feet. On the following day you shall again go to the treasury, take a coin worth 2 brasses and place it here near the first one. On the third day you are to bring a coin worth 4 brasses and on the fourth day bring a coin worth 8 brasses, on the fifth, 16, etc., double the value of the previous coin. I will order appropriate coins be produced for you and while you have the strength, you will take them from my treasury. Nobody may help you, you must rely on your own power only. You will stop when you notice that cannot move a coin any more and then our deal will come to an end. All the coins that you will have managed to bring here will belong to you and you shall keep them as your reward.” Terentius listened eagerly to the Emperor’s words. He visualized the multitude of coins, each one more than another, that he would bring out of the treasury. “I’m happy with your favour,” he beamed. “Really generous is your reward!” III. Terentius started his daily visits to the treasury. It was located close to the Emperor’s hall so the first trips with the coins cost Terentius very little effort. On the first day he only brought 1 brass. This was a small coin 21 millimetres across and weighing 5 grammes. His trips upto the sixth day were also very easy and he brought the coins double, fourfold, sixteen-fold, and thirty-two-fold the weight of the first. * A brass is a fifth of a denarius. 238-239 Stories about Giant Numbers The seventh coin weighed 320 grammes and was 8 1/2 centimetres across.* On the eighth day Terentius had to carry out a coin that was worth 128 units. It weighed 640 grammes and was about 10 1/2 centimetres wide. On the ninth day he carried into the Emperor’s hall a coin corresponding to 256 unit coins. It was 13 centimetres wide andweighed more than 1 1/4 kilogrammes. On the twelfth day the coin was almost 27 centimetres across and 10 1/4 kilogrammes in weight. The Emperor who up until that day was very kind to the general now couldn’t conceal his triumph. He saw that after 12 days only slightly more than 2,000 brass units had been brought. Further, on the thirteenth day the brave Terentius brought out a coin that was worth 4,096 units. It was 34 centimetres wide and weighed 20 1/2 kilogrammes. On the fourteenth day Terentius had a heavy coin that was 42 centimetres across and weighed 41 kilogrammes. “Are you tired, my brave Terentius?” the Emperor could hardly help smiling. “No, Sire,” the general responded grimly wiping his brow. The fifteenth day came. This time Terentius’s burden was really heavy. He trudged slowly to the Emperor carrying a huge coin corresponding to 16,384 unit coins. It was 53 centimetres wide and weighed 80 kilogrammes, the weight of a tall warrior. On the sixteenth day the general staggered with the burden on his back. It was a coin equal to 32,768 units, its diameter being 67 centimetres and weighing 164 kilogrammes. The general was exhausted and gasping. The Emperor smiled... When Terentius came to the Emperor the next day, there was a roar of laughter. He could no longer carry his coin in his hands and rolled it in front of him. The coin was 84 centimetres and 328 kilogrammes, and corresponded to 65,536 unit coins. The eighteenth day was the last day of Terentius’s enrichment, for his visits to the treasury and trips to * If a coin’s volume is 64 times that of a normal one, then it is only four times wider and thicker, because 4 x 4 x 4 = 64. We should have this in mind when working out the sizes of further coins. Stories about Giant Numbers the Emperor’s hall ended on that day. This time he had to fetch a coin worth 131,072 unit coins. It was more than a metre across and weighed 655 kilogrammes. Using his spear as a lever Terentius rolled it into the hall with a huge effort. The mammoth coin fell thundering at the Emperor’s feet. Terentius was completely worn out. “Can’t do any more... Enough for me,” he wispered. The Emperor could hardly conceal his pleasure at the total triumph of his ruse. He ordered the treasurer to compute the total of all the brasses brought into the hall by Terentius. The treasurer reckoned quickly and said: “Sire, thanks to your generosity the victorious warrior Terentius has got a reward of 262,143 brasses.” So the close-fisted Emperor gave the general about 1/20 part of the million of denarii Terentius had requested. * * * Let’s check the treasurer’s calculation and the weight of the coins. Terentius brought out: Day Coin Weight in brasses in grammes 1 1 5 2 2 10 3 4 20 4 8 40 5 16 80 6 32 160 7 64 320 8 128 640 9 256 1,280 10 512 2,560 11 1,024 5,120 12 2,048 10,240 13 4,096 20,480 14 8,192 40,960 15 16,384 81,920 16 32,768 163,840 17 65,536 327,680 18 131,072 655,360 The totals for these columns can be calculated easily using the proper rule*, thus the second column totals * Each number in this column equals the sum of the previous ones plus one. Therefore, when it’s necessary to sum up all the numbers in the column, e. g. from 1 to 32,768, we need only find the next number and subtract one, i.e. 32,768 x 2— 1. The result is 65,535. 240-241 Stories about Giant Numbers 262,143. Terentius requested a million of denarii, i.e. 5 million brasses. Accordingly, he got 5,000,000 -i- 262,143 = 19 times less than he requested. Legend about Chess-Board I. Chess is one of the world’s most ancient games. It has been in existence for centuries so it is no wonder that it has given rise to many legends whose truth¬ fulness cannot be checked because of the remotedness of the events. One of these legends I want to relate. You do not need to be able to play chess to understand it, it is sufficient for you to know that it involves a board divided into 64 cells (black and white alternately). The play of chess was invented in India. When the Indian king Sheram got to know about it he was amazed at its ingeniousness and the infinite variety of positions it afforded. Having learned that the play was invented by one of his subjects, the king summoned him in order to reward him personally for such a stroke of brilliant insight. The inventor, named Seta, came before the sovereign’s throne. He was a simply dressed scribe who earned his living giving lessons to pupils. Stories about Giant Numbers “I want to reward you properly, Seta, for the beaut¬ iful play you invented,” the king said. The sage bowed. “I’m rich enough to fulfil any of your desires,” the king went on to say. “Name a reward that would satisfy you and you’ll get it”. There was a silence. “Don’t be shy! What’s your desire? I’ll spare nothing to meet your wish!” “Great is your kindness, oh sovereign. Give me some time to sleep on it. Tomorrow, upon consideration. I’ll name you my wish.” When the next day Seta came to the throne he amazed the king by the unprecedented modesty of his desire. Seta said: “Sovereign, order that one grain of wheat be given to me for the first cell of the chess-board.” “A simple wheat grain?” the king was shocked. “Yes, sovereign. For the second cell let there be two grains, for the third four, for the fourth eight, for the fifth 16, for the sixth 32...” “Enough!” the king was exasperated. “You’ll get your grains for all the 64 cells of the board according to your wish: for each twice as much as for the previous one. But let me tell you that your wish is unworthy of my generosity. By asking for such a miserable reward you show disrespect for my favour. Truly, as a teacher you might give a better example of gratitude for the kindness of your king. Go away! My servants will bring you the bag of wheat.” Seta smiled, left the hall and began to wait at the palace gates. II. At dinner the king remembered about the inventor of chess and asked if the foolish Seta has collected his miserable reward. The answer was: “Sovereign, your order is being fulfilled. The court mathematicians are computing the number of grains required.” The king frowned-he wasn’t used to having his orders fulfilled so slowly. At night, before going to bed the king Sheram again inquired how long before had Seta left the palace with his bag of wheat. “Sovereign, your mathematicians are working hard and hope to finish their calculations before dawn.” “Why so long?” the king was furious. “Tomorrow, 242-243 Stories about Giant Numbers before I wake up everything, down to the last grain, must be given to Seta. I never give my order twice!” First thing in the morning the king was told that the chief mathematician humbly asked to make an important report. The king ordered him in. Sheram said: “Before you bring out your business I’d like to know if Seta has at last received the miserable reward that he asked for.” The old man responded: “It’s exactly because of this that I dared to bother you at such an early hour. We’ve painstakingly worked out the number of grains that Seta wants to have. The number is so enormous...” “No matter how enormous it is”, the king interrupted him arrogantly, “my granaries won’t be depleted! The reward is promised and must be given out...” “It’s beyond your power, oh sovereign, to fulfil his wish. There is not sufficient grain in all your barns to give Seta what he wants. And there is not enough in all the bams throughout the kingdom. You would not find that many grains in the entire space of the earth. And if you wish to give out the promised reward by all means, then order all the kingdoms on earth to be turned into arable fields, order all the seas and oceans dried up, and order the ice and snowy wastes that cover the far northern lands melted. Should all the land besown with wheat and should the entire yield of these fields be given to Seta, then he’d receive his reward.” The king attended to the words of the elder with amazement. “What is this prodigious number?” “18,446,744,073,709,551,615, oh sovereign!” III. Such was the legend. There is now no way of knowing if it’s true, but that the reward is expressed by this number you could verify by some patient calculations. Starting with unity you’ll have to add up number 1,2,4,8, etc. The result of the 63th doubling will be what the inventor should receive for the 64th cell of the board. If you use the rule explained at the end of the previous problem, you can easily obtain the number of grains to be received by the inventor (we double the last number and subtract one). Hence the calculation comes down to multiplying together 64 twos: 2x2x2x2x2, etc.,-64 times. 16* Stories about Giant Numbers To facilitate computation divide the 64 multipliers into six groups with 10 twos in each and one last group with four twos. It’s easy to see that the product of 10 twos is 1,024, and of four twos, 16. The desired result is thus 1,024 x 1,024 x 1,024 x 1,024 x 1,024 x 1,024 x 16. Multiplying 1,024 x 1,024 gives 1,048,576. It now remains to find 1,048,576 x 1,048,576 x x 1,048,576 x 16, subtract one from the result to arrive at the sough t-for number of grains: 18,446,744,073,709,551,615. If you want to imagine the enormousness of this numerical giant just estimate the size of a barn that would be required to house this amount of grain. It’s known that a cubic metre of wheat contains about 15,000,000 grains. Consequently, the reward of the inventor of chess would occupy about 12,000,000,000,000 cubic metres, or 12,000 cubic kilometres. If the barn were 4 metres high and 10 metres wide its length would be 300,000,000 kilometres, twice the distance to the Sun! The Indian king could never grant such a reward. Had he been good at maths, he could have freed him¬ self of the debt. He should have suggested to Seta to count off the grains he wanted himself. In fact, if Seta kept on counting day in day out he would have counted only 86,400 grains in the first 24 hours. A million would have required no less than 10 days of continual reckoning and thus to process 1 cubic metre of wheat would have required about half a year. In a ten year’s time he would have handled about 20 cubic metres. You see that even if Seta had devoted a lifetime to his counting, he would still have only obtained a miserable fraction of the reward he desired. Prolific Multiplication A ripe poppy head is full of tiny seeds, each of which can give rise to a new plant. How many poppy plants shall we have, if all the seeds germinate? To begin with we should know how many seeds there are in a head. A boring business, but if you summon up all your patience you’ll find that one head contains about 3,000 seeds. What follows from this? If there is enough space around our poppy plant with adequate soil, each seed will produce a shoot with the result that the following 244-245 Stories about Giant Numbers summer 3,000 poppies will grow. A whole poppy field from just one head. Let’s see what will happen next. Each of the 3,000 plants will produce no less than one head (more often several heads), with 3,000 seeds each. Having germinated, the seeds of each head will give 3,000 new plants, and hence during the following year we are going to have 3,000 x 3,000 = 9,000,000 plants. Calculation gives that in the third year the offspring of our initial head will already reach 9,000,000 x 3,000 = 27,000,000,000. In the fourth year there will be 27,000,000,000 x 3,000 = 81,000,000,000,000 offspring. In the fifth year our poppies will engulf the earth, because they’ll reach the number 81,000,000,000,000 x 3,000 = 243,000,000,000,000,000. But the surface area of all the land, i.e. all the continents and islands of the earth, amount to 135,000,000 square kilometres, or 135,000,000,000,000 square metres-about 2,000 times less than the number of the poppy plants grown. You see thus that if all the poppy-seeds from one head germinated, the offspring of one plant could engulf the earth in five years so that there were about 2,000 plants of each square metre of land. Such a numerical giant lives in a tiny poppy seed! A similar calculation made for a plant other than the poppy, one which yields less seeds, would lead to the same result with the only distinction that its offspring would cover the lands of the earth in a longer period than five years. Take a dandelion, say, which gives about 100 seeds annually. Should all of them germinate, we would have: Year 1 2 3 4 5 6 7 8 9 Number of plants 1 100 10,000 1,000,000 100,000,000 10,000,000,000 1,000,000,000,000 100,000,000,000,000 10,000,000,000,000,000 Stories about Giant Numbers This is 70 times more than the square metres of land available on the globe. In consequence, the whole Earth would be covered by dandelions in the ninth year with about 70 plants on each square metre. Why then don’t we observe in reality these tremendous multiplications? Because the overwhelming majority of seeds die without producing any new plants, they either fail to hit a suitable patch of soil and don’t germinate at all, or having begun to germinate are suppressed by other plants, or are eaten by animals. If there were no massive destruction of seeds and shoots, any plant would engulf our planet in a short period. This is true not only of plants but of animals, too. If it were not for death, the offspring of just one couple of any animal would sooner or later populate all the land available. Swarms of locust covering huge stretches of land may give some idea of what might happen on earth if death didn’t hinder the multiplication of living things. In two decades or so the continents would be covered with impenetrable forests and steppes inhabited by incountable animals struggling for their place under the sun. The oceans would be filled to the brim with fish so that any shipping would be impossible. And the air would not be transparent because of the mists of birds and insects... Before we leave the subject, we’ll consider several real-life examples of uncannily prolific animals placed in favourable conditions. At one time America was free of sparrows. The bird that is so common in Europe was deliberately brought to the United States to have it exterminate the destructive insects. The sparrow is known to eat in quantity voracious caterpillars and other garden and forest pests. The sparrows liked their new environment, since there were no birds of prey eating them, and so they began to multiply rapidly. The number of insects began to drop markedly and before long the sparrows, for want of animal food, switched to vegetable food and went about destroying crops*. The Americans were even forced to initiate a sparrow control effort which appeared to be so expensive that a law was passed forbidding the import to America of any animals. * In the Hawaii they even completely superseded small endemic birds. 246-247 Stories about Giant Numbers A further example. There were no rabbits in Australia when the continent was colonized by the Europeans. The rabbits were brought to Australia in the late 18th century and as there were no carnivores that might be their enemies they began to multiply at a terrifically fast rate. Hordes of rabbits soon inundated Australia inflicting enormous damage to agriculture. They became a plague of the country and their eradication required great expense and effort. Later the same situation with rabbits occurred in California. A third instructive story comes from Jamaica. The island was suffering from an abundance of poisonous snakes. To get rid of them it was decided to introduce the secretary-bird, an inveteratekiller of poisonous snakes. The number of snakes soon dropped all right, but instead the island got to be infested with the rats that earlier were controlled by the snakes. The rats wrought dreadful havoc amongst the sugar cane fields and posed an urgent problem. It’s known that an enemy of the rats in the Indian mongoose, and so it was decided to bring four pairs of these animals to the island and allow them multiply freely. The mongooses adapted perfectly to their new land and in a short period of time inhabited the island. In less than a decade they had almost wiped out the rats. But alas, having destroyed the rats, the mongooses began to consume whatever came their way and turned into omnivores. They started killing puppies, goat-kids, piglets, poultry. And when they had multiplied still fur¬ ther they set about devastating orchards, fields and plantations. So the inhabitants of the island were compelled to start combating their previous allies, but with limited success. Free Dinner Ten young people decided to celebrate leaving school by a dinner at a restaurant. When all had gathered they started arguing as to how they were to sit at the table. Some suggested that they sit in alphabetic order, others, by age, yet others, by their academic record, or even by their height. The argument dragged on, but nobody sat down at the table. It was the waiter who made it up between them. He said: “My young friends, you’d better stop arguing, sit at Stories about Giant Numbers the table arbitrarily and listen to me.” The ten set anyhow and the waiter continued: “Let somebody record the order in which you are sitting now. Tomorrow come here again to dine and sit in another order. The day after tomorrow you sit in a new order, and so on, until you have tried out all the arrangements possible. When you come to sit in exactly the same order as you are sitting now, then upon my word, I’ll start to treat you to the finest dinners without charge.” The party liked the suggestion. It was decided to come every night and try all the ways of sitting at the table in order to enjoy the free dinner as soon as possible. They didn’t live to see it, however. And not because the waiter didn’t keep his word, but because the number of arrangements was too great. Specifically, it is 3,628,800. You can see this number of days equals to almost 10,000 years! It might seem unlikely to you that as few as 10 people might be arranged in such an enormous number of various ways but we can check it. To begin with, we must learn how to find the number of permutations possible. To make our life easier we’ll begin with a small number of objects, say three. Let’s label them A, B, and C. We would like to know in how many ways it’s possible to permute them. We argue as follows: if for the moment we put B aside, the two remaining objects may be arranged in two ways. We will now attach B to each of the two pairs. We may place it in each of three ways: (1) B behind the pair; (2) B in front of the pair; (3) B between the members of the pair. Clearly, there are no other positions for B besides these three. But as we have two pairs, AB and BA, then there are 2x3 = 6 ways of arranging the objects. Further, we’ll repeat the argument for four objects. Let there be four objects A, B, C, and D. We’ll again put aside one object and make all the possible permutations with the remaining three. We know already that there are six of these. In how many ways may we attach D to each of the six arrangements of three? Obviously, we may place it as follows; (1) D behind the triple; (2) D in front of the triple; 248-249 Stories about Giant Numbers (3) D between the first and second objects; (4) D between the second and third objects. We thus get 6 x 4 = 24 permutations, and since 6 = = 2x3, and 2=1x2, then the number of permutations may be represented as the product 1 x x 2 x 3 x 4 = 24. Reasoning along the same lines we’ll find that for five objects, too, the number of permutations is 1 x 2 x 3 x x 4 x 5 = 120. For six objects: Ix2x3x4x5x6 = 720, and so on. Return now to the case of the 10 diners. The number of permutations possible here is obtainable if we take the trouble of multiplying together Ix2x3x4x5x x6x7x8x9xl0. This will in fact give the above-mentioned 3,628,800. The calculation would be more complex if among the 10 diners there were five girls who wanted to alternate with the boys. Although the number of the possible permutations is far less in this case, it’s somewhat more difficult to work it out. Let one boy seat at the table somewhere. The remaining four may only be seated in alternate chairs (leaving the vacant places for the girls) in 1 x 2 x 3 x x 4 = 24 various ways. Since the total number of chairs is 10, the first boy may be seated in 10 ways, hence the number of all possible arrangements for the boys is 10 x 24 = 240. What is the number of ways in which the five girls may occupy the vacant chairs between the boys? Clearly, 1 x2x3x4x5 = 120. Combining each of the 240 positions for the boys with each of the 120 positions of the girls we obtain the number of all the possible arrangements: 240 x 120 = 28,800. The above number is smaller by far than the previous one though it would require almost 79 years to work through them all. Should the young guests of the restaurant live to be 100, they could get the free dinner, if not from the waiter himself, then from his successor. 18 T] Tricks with Numbers Out of Seven Digits Write the seven digits from 1 to 7 one after the other: 1 2 3 4 5 6 7. It’s easy to connect them by the plus and minus signs to obtain 40, e. g. 12 + 34 - 5 + 6 - 7 = 40. Try and find another combination of these digits that would yield 55. Nine Digits Now write out the nine digits: 12345678 9. You can as above arrive at 100 by inserting a plus or minus six times and get 100 thus: 12 + 3- 4 + 5 + 67 + 8 + 9= 100. If you want to use only four plus or minus signs, you proceed thus: 123 + 4 - 5 + 67 - 89 = 100. Now try and obtain 100 using only three plus or minus signs. It’s much more difficult but possible. With Ten Digits Obtain 100 using all ten digits. In how many ways can you do it? There are no less than four different ways. Unity Obtain unity using all ten digits. With Five Twos We only have five twos and all the basic mathematical operation signs at our disposal. Use them to obtain the following numbers: 15, 11, 12, 321. Once More with Five Twos Is it possible to obtain 28 using five twos? 250-251 Tricks with Numbers With Four Twos The problem is more involved. Use four twos to arrive at 111. Is that possible? With Five Threes To be sure, with the help of five threes and the mathematical operation signs we can represent 100 as follows: 33 x 3 + y = 100. But can you write 10 with five threes? The Number 37 Repeat the above problem to obtain 37. In Four Ways Represent 100 in four various ways with five identical digits. With Four Threes The number 12 can be very easily expressed with four threes: 12 = 3 + 3 + 3 + 3. It’s more of a problem to obtain 15 and 18 using four threes: 15 = (3 + 3)+ (3x3); 18 = (3 x 3) + (3 x 3). And if you were required to arrive at 5 in the same way, you might be not very quick to twig that 5 = Now think of the ways to get the numbers 1, 2, 3, 4, 6, 7, 8, 9, 10. With Four Fours If you have done the previous problem and want some more in the same vein, try to arrive at all the numbers Tricks with Numbers from 1 to 10 with fours. This is no more difficult than getting the same numbers with the threes. With Four Fives Obtain 16 using four fives. With Five Nines Can you provide at least two ways of getting 10 with the help of five nines? Twenty-Four It’s very easy to obtain 24 with three eights: 8 + 8 + 8. Could you do thisThey huddled together, and waited; and he climbed down, and came in. “He was a young keeper, as luck would have it, and new to the business; and when he got in, he couldn’t get to them, and then he got lost. They caught sight of him, every now and then, rushing about the other side of the hedge, and he would see them, and rush to get to them, and they would wait there for about five minutes, and then he would reappear again in exactly the same spot, and ask them where they had been. “They had to wait until one of the old keepers came back from his dinner before they got out.” “They were a bit dense,” I said, “To have a plan and Bay the Way Figure 12 not to find the way out.” “Do you think you’d find at once?” “With a plan? Certainly!” “Just wait. It seems to me I’ve got the plan of that maze,” Alex said and began to delve in his bookcase. “Does this maze really exist?” “Hampton Court? Of course, it’s near London. Been in existence for two centuries... Found at last. Just as I said Plan of the Maze at Hampton Court. It seems rather small, this maze, only 1,000 square metres.” My brother opened the book at a page showing a small plan. “Imagine you’re here in the central area of the maze and want to get out, which way would you go to get to the exit? Sharpen a match and use it to show the way.” I pointed the match at the centre of the maze and bravely drew it along the winding paths of the maze, but the whole affair appeared to be more involved than I had expected. Having wandered a little round about the plan I came... back to the central area, just as Jerome’s characters had, the ones I’d just made fun of! “You see, the plan is no use. But rats solve the task without any plan.” “Rats? What rats?” “The ones described in this book. Do you think this is a treatise on garden design? No, this book is about the mental abilities of animals. To test the intelligence of animals, scientists make a small plaster model of a maze and put the animals to be tested into it. The book says that rats can find their way about a plaster maze of Hampton Court in only half an hour and that is faster than the people in Jerome’s book.” 48-49 By the Way “Judging from the plan, the maze doesn’t seem to be very difficult. You would never think that it’s so treacherous...” “There’s a simple rule. If you know it, you can safely enter any maze without any fear of getting lost.” “Which rule?” “You should follow the paths touching its wall with your right hand, or left for that matter-it makes no difference. But with one hand, all the time.” “Just this?” “Yes. Now try and use the rule in reality, mentally wandering about the plan.” I ran my match along the paths, being guided by the rule. Truly, I soon came from the entrance to the centre and back again, to the exit. “A beautiful rule.” “Not really,” Alex objected, “The rule is good so long as you simply don’t want to be lost in a maze, but it’s no good if you want to walk along all of its paths without exception.” “But I’ve just been in all the alleys on the plan. I didn’t miss one.” “You are mistaken. Had you marked with a dash line the way you went, you’d have found that one alley wasn’t covered.” “Which one?” Figure 13 “I’ve marked it with a star on this plan (Fig. 13). You haven’t been down this alley. In other mazes the rule would guide you past large sections of it so that even though you’d find your way out safely, you wouldn’t see much of it.” “Are there many different kinds of maze?” “A lot. Nowadays they are only in garden and parks and you wander around in the open air between high green walls of hedge, but in ancient times they used to put mazes inside large houses or dungeons. That was 4-621 By the Way done with the cruel aim of dooming the unhappy people thrown into them to wander hopelessly about the intricate tangle of corridors, passages and halls, eventually leading them to starve to death. One such, for instance, was the proverbial maze on the island of Crete and the legend has it that an ancient king called Minos had it built. Its paths were so tangled that its own creator, a man called Daedalus, allegedly couldn’t find his way out of it,” brother continued, “The aim of other ancient mazes was to guard the tombs of kings, to protect them from robbers. A tomb was located at the centre of a maze so that if a greedy seeker after buried treasure even succeeded in reaching it, he wouldn’t be able to find his way out-the grave of the king would become his grave, too.” “Why didn’t they use the rule for walking round mazes you’ve just told me about?” “For one thing, apparently, in ancient times nobody knew about the rule. For another. I’ve already told you that it doesn’t always let you visit every part of the maze. A maze can be contrived in such a way that the user of the rule will miss the place where the treasure is kept.” “But is it possible to make a maze from which there is no escaping? Of course, someone who enters it using your rule will get out eventually, but suppose a man is put inside and left there to wander?” “The ancients thought that when the paths of a maze are sufficiently tangled, it would be absolutely impossible to get out of it. This isn’t true because it can be proved mathematically that inescapable mazes cannot be built. Not only that but every maze has an escape and it is possible to visit every corner without missing one and still escape to safety. You only need to follow a strict system and take certain precautions. Two centuries ago the French botanist Tournefort dared to visit a cave in Crete which was said to be an inescapable maze because of its innumerable paths. There are several such caves in Crete and it may be possible that they gave rise to the ancient legend about the maze of King Minos. What did the French botanist do in order not to be lost? This is what his fellow-countryman, the mathematician Lucas, said about it.” My brother took down from the bookcase an old book entitled Mathematical Amusements and read aloud the following passage (I copied it later): “Having wandered for a time with our companions 50-51 By the Way Figure 15 Figure 16 about a network of underground corridors, we came to a long wide gallery that led us into a spacious hall deep in the maze. We had counted 1460 steps in half an hour along this gallery, deviating neither right nor left... On either side there were so many corridors that one would be bound to get lost there unless some necessary precautions were taken. But as we had a strong desire to be out of the maze, we saw to it to provide for our return. “First, we left one of our guides at the entrance to the cave, having instructed him to call for the people from a neighbouring village to rescue us should we not return by night fall. Second, each of us had a torch. Third, at every turn which, it seemed, might be difficult to find later we attached numbered papers to the wall. Finally, one of our guides put on the left side bunches of blackthorn he had prepared beforehand, and the other side of the path he sprinkled with chopped straw, which he carried in a bag.” Alex finished reading and said, “All these laborious precautions might not seem all that necessary to you. In the times of Tournefort, however, there was no other way since the problem of mazes had not yet been solved. These days the rules for walking around mazes have been worked out that are less burdensome but no less reliable than his precautions.” “Do you know these rules?” “They aren’t complicated. A first rule is that when you walk into a maze, follow any path till you reach a dead end or a crossing. If it is a dead end, return and place two stones at the exit which will indicate that the corridor has been passed twice. At a crossing, go fur¬ ther down any corridor but mark each time you go down it with a stone theusing other sets of three identical digits? The problem has several solutions. Thirty The number 30 can easily be expressed with three fives: 5x5 + 5. It’s more difficult to do this with other sets of identical digits. Try it, you’ll may be able to find several solutions. One Thousand Could you obtain 1,000 with the aid of eight identical digits? Get Twenty The following are three numbers written one below the other: 111 111 999 Try and cross out six digits so that the sum of the remaining numbers be 20. Cross out Nine Digits The following columns of five figures each contain 15 odd digits: 252-253 THcks with Numbers 1 1 1 3 3 3 5 5 5 111 9 9 9 The problem is to cross out nine digits so that the numbers thus obtained add up to 1,111. In a Mirror The number corresponding to a year of the last century is increased 41/2 times if viewed in a mirror. Which year is it? Which Year? In this century, is there a year such that the number expressing it doesn’t change if viewed “upside down”? Which Numbers? Which two integers, if multiplied together, give 7? Don’t forget that both numbers should be integers, therefore answers like 31/2x2 or 21/3x3 won’t do. Add and Multiply Which two integers, if added up, give more than if multiplied together? The Same Which two integers, if multiplied together, give the same as if added up? Even Prime Numbers You must know that prime numbers are those that are divisible without remainder by themselves only or by unity. Other numbers are called composite. What do you think: are all the even numbers composite? Are there any even prime numbers? Three Numbers Which three integers, if multiplied together, give the same as if added up? Tricks with Numbers Addition and Multiplication You’ve undoubtedly noticed the curious feature of the equalities: 2 + 2 = 4, 2x2 = 4. This is the only case where the sum and product of two integers (equal to each other at that) are equal. You maybe are unaware that there are dissimilar numbers showing the same property. Think of examples of such numbers. So that you don’t believe that the search would be in vain I assure you that there are many such number pairs, though none of them are integers. Multiplication and Division Which two integers yield the same result whether the larger of them is divided by the other or they are multiplied together? The Two-Digit Number There is a two-digit number such that if it is divided by the sum of its digits the answer is also the sum of the digits. Find the number. Ten Times More The numbers 12 and 60 have a fascinating property: if we multiply them together, we get exactly 10 times more than if we add them up: 12 x 60 = 720, 12 + 60 = 72. Try and find another pair like this. Maybe you can find several pairs with the same property. Two Digits What is the smallest-positive integer that you could write with two digits? The Largest Number What is the largest number that you can write with four ones? 254-255 Dricks with Numbers Unusual Fractions Consider the fraction 6729/13,458. All the digits (save for 0) are used in it once. As is easily seen, the fraction is 1/2. Use the nine digits to obtain the following fractions: 1111111 T T’ 5~’ ~6’ V ¥’ 9“' What Was the Multiplier? A schoolboy carried out a multiplication, then rubbed most of his figures from the blackboard so that only the first line of the figures and two digits in the last line survived. As to the other figures, only the following traces remained: 235 x ** **** + **** **56* Could you restore the multiplier? Missing Figures In this multiplication case more than half the figures are replaced by asterisks: *1* x 3*2 *3* 3*2* + *2*5 1*8*30 Can you restore the missing figures? What Numbers? A further problem of the same sort: Tricks with Numbers **5 X 1** 2**5 + 13*0 *** 4*77* Strange Multiplication Cases Consider the following case of the multiplication of two numbers: 48 x 159 = 7,632. It’s remarkable in that each of the nine digits is involved once here. Can you think of any other examples? If so, how many of them are there? Mysterious Division What is given below is nothing but an example of a long-division sum where all the digits are replaced by points: . . . 7 . • • • T Not one digit in either the dividend or the divisor is known. It’s only known that the last but one digit in the quotient is 7. Determine the result of the division. The problem has only one answer. 256-257 Tricks with Numbers Another Division Problem Restore the missing figures in the division below: _1^ 325) *2*5* *** *0** *g** Figure 230 Figure 231 *5* *5* Division by 11 Write out a nine-digit number containing no repeated digits (all the digits are different), that divides by 11 without remainder. What is the largest such number? What is the smallest such number? Triangle of Figures Within the circles of the triangle of Fig. 230 arrange all the nine digits so that the sum of the digits on each side be 20. Another Triangle Repeat the previous problem so that each side adds up to 17. Eight-Pointed Star Into the circles of the figure of Fig. 231 insert one of the numbers from 1 to 16 so that the sum of the numbers on the side of each square be 34 and the sum of the numbers at the comers of each square be 34, too. Magic Star The six-pointed star shown in Fig. 232 is “magic” because all the six lines of numbers have the same sum: 4 + 6+ 7 + 9 = 26, 11 + 6+ 8+ 1 =26, 4 + 8 + 12 + 2 = 26, 11+ 7+ 5 + 3 = 26, 9 + 5 + 10 + 2 = 26, 1 + 12 + 10 + 3 = 26. 17-621 Tricks with Numbers Figure 233 Figure 234 However the numbers at the points of the star add up to another number: 4 +11+9 + 3 + 2+1 = 30. Couldn’t you improve the star so that the numbers at the points also gave the same sum (26)? Wheel of Figures The digits from 1 to 9 should be so arranged in the circles of the wheel of Fig. 233 that one digit is at the centre and the others elsewhere about the wheel so that the three figures in each line add up to 15. Trident It’s required to arrange the numbers from 1 to 13 in the cells of the trident shown in Fig. 234 so that the sums of the figures in each of the three columns (I, II, and III) and in the line (IV) are the same. Answers 258-259 »=o Out of Seven Digits There are three solutions: 123 + 4-5-67 = 55; 1 -2-3-4 + 56 + 7 = 55; 12 - 3 + 45 - 6 + 7 = 55. Nine Digits 123 - 45 - 67 + 89 = 100. This is the only solution. It’s impossible to arrive at the same result by using the plus and minus signs less than three times. With Ten Digits The following are the four solutions: 70 + 24-^-+ 5 \ =100; 18 6 27 3 80——+ 19 — = 100; 54 6 84+9t+3w-100; 1 38 50 —+ 49 —= 100. 2 76 Unity Represent unity as the sum of two fractions: 148 35 _ 296 +W ‘ Those knowing more advanced mathematics may also give other answers: 123,456,789°; 234,5679 “ 8 " \ etc., since any number to the zeroth power is unity. Answers And 11 as: With Five Twos Write 15 as: (2 + 2)2 — y = 15; -y- + 2 x 2 = 15; (2 x 2)2 — y = 15; -y- + 22 = 15; 2-|=15; ^- + 2 + 2=15. 22 + 2-2 = 11. Now the number 12,321. At first sight, it would seem impossible to write this five-digit number with five similar figures. The problem is manageable, however. Here is the solution: 222 ~T~ = 1112 = 111 x 111 = 12,321. Once More with Five Twos 22 + 2 + 2 + 2 = 28. With Four Twos The solution is: With Five Threes 33 3 It’s worth mentioning that the problem would have had exactly the same solution if we had had to express 10 with five ones, five fours, five sevens, five nines, or, in general, with any five identical digits. In fact: U__J__22_.2_44_4__99_9^ T_7-”2~_7__4~ 7-~9 7’ etc' 260-261 Answers Also, there areway you have just passed and the way you are going to follow. A second rule states that having arrived along a fresh corridor at a crossing that has earlier been visited (as seen by the stones), go back at once and place two stones at the end of the corridor. Finally, a third rule requires that having come to a visited crossing along a corridor that has already been walked, mark the way with a second stone and go along one of new corridors. If there doesn’t happen to be such a corridor, take one whose entrance has only one stone (that is a corridor that has only been passed once). Abiding by these rules you can pass twice, that is there and back, every corridor of the maze without missing any comer and return back to safety. Here I’ve 4* By the Way got several plans of mazes I’ve cut out at different times from illustrated magazines (Figs. 14, 15, and 16). If you wish, you can try and travel about them. I hope that now that you know so much you shouldn’t be in any danger of getting lost in them. If you’ve enough patience, you could actually make a maze like, say, the Hampton Court one that Jerome mentioned-you could construct it with your friends out of snow in the yard.” 52-53 For Young Physicists Figure 17 More Skilled Than Columbus A schoolboy once wrote in a composition: “Christo¬ pher Columbus was a great man because he discovered America and stood an egg upright.” This young scholar had thought both deeds equally amazing. On the contrary, the American humorist Mark Twain saw nothing special about Columbus discovering America: “It would have been strange if he hadn’t found it there.” The other feat the great navigator had performed is not really all that marvellous. Do you know how Columbus stood an egg upright? He simply pressed it down onto a table crushing the bottom of the shell. He had, of course, changed the shape of the egg. But how can one possibly stand an egg on end without changing its shape, the navigator didn’t know. Meanwhile it is easier by far than discovering America or even one tiny island. I’ll show you three methods: one for boiled eggs, one for raw eggs, and one for both. A boiled egg can be stood upright simply by spinning it with your fingers or between your palms like a top. The egg will remain upright as long as it spins. After two or three trials the experiment should come out well. This won’t work if you try to stand a raw egg up¬ right, you may have noticed that raw eggs spin poorly. This, by the way, is used to distinguish a hard-boiled egg from a raw one without breaking the shell. The liquid contents of a raw egg is not carried along by the spinning as fast as the shell and, therefore, sort of damps the speed down. We have to look for another way of standing eggs and one does exist. You have to shake an egg intensely several times. This breaks down the soft envelope containing the yolk with the result that the yolk spreads out inside the egg. If you then stand the egg on its blunt end and keep it this way for a while, then the yolk, which is heavier than the white, will pour down to the bottom of the egg and concentrate there. This will bring the centre of mass of the egg down making it more stable than before. Finally, there is a third way of putting an egg up¬ right. If an egg is placed, say, on the top of a corked bottle and another cork with two forks stuck into it is placed on the top as shown in Fig. 17, the whole For Young Physicists Figure 18 Figure 19 Figure 20 system (as a physicist would put it) is fairly stable and remains in equilibrium even if the bottle is slightly inclined. But why don’t the egg and cork fall down? For the same reason that a pencil placed upright on a finger doesn’t fall off when a bent penknife is stuck into it as shown. A scientist would explain: “The centre of mass of the system lies below the support.” This means that the point at which the weight of the system is applied lies below the place at which it is supported. Centrifugal Force Open an umbrella, put its end on the floor, spin it and drop a ball into it. The ball could be a balled piece of paper or handkerchief, or any other light and unbreakable thing. Something will happen you probably wouldn’t expect. The umbrella does not, as it were, desire to accept the present and the thing itself crawls up the edge and then flies off in a straight line. The force that threw the ball out in this experiment is generally called the “centrifugal force”, although it would be more appropriate to dub it “inertia”. Centrifugal force manifests itself when a body travels in a circle but this is nothing but an example of inertia which is the desire of a moving body to maintain its speed and direction. We come across centrifugal force more often than you might suspect. If you whirl a stone tied to a piece of string, you can feel the string become taut and seem to be about to break under the action of the centrifugal force. The ancient weapon for hurling stones, the sling, owes its existence to the force. Centrifugal force bursts a millstone, if it is spun too fast and is not sufficiently strong. If you are adroit enough, this force will help you to perform a trick with a glass from which the water doesn’t escape, even though it is upside down. In order to do this you’ll only have to swing the glass quickly above your head in a circle. Centrifugal force helps a circus bicyclist to do a “devil’s loop”. It is put to work. In the so-called centrifugal separators it churns cream; it extracts honey from honey-comb; it dries washing by extracting water in centrifugal driers, etc., etc. When a tram travels in a circular path, e.g. as it turns at a crossing, the passengers feel directly the centrifugal force that pushes them in the direction of the outer wall of the carriage. If the speed is sufficiently 54-55 For Young Physicists large, the carriage could be overturned by the force if the outer rail wasn’t laid a bit higher than the inner one: which is why a tram is slightly inclined inwards when it turns. It sounds rather unusual but an inclined tram is more stable than an upright one! But this is quite the case, though. A small experiment will help explain this to you. Bend a cardboard sheet to form a wide funnel, or better still take a conical bowl if available. The conical shield (glass or metallic) of an electrical lamp would be suitable for our purposes. Roll a coin (small metal disk, or ring) around the edge of any of these objects. It will travel in a circle bending in noticeably on its way. As the coin slows down, it will travel in ever decreasing circles approaching the centre of the funnel. But by slightly shaking the funnel the coin can easily be make roll faster and then it will move away from the centre describing increasingly larger circles. If you overdo it a bit, the coin will roll out. For cycling races in a velodrome special circular tracks are made and you can see that these tracks, especially where they turn abruptly have a noticeable slope into the centre. A cyclist rides along them in an inclined position (like the coin in the funnel) and not only does he not turn over but he acquires special stability. Circus cyclists used to amaze the public by racing along a steep deck. Now you can understand that there is nothing special about it. On the contrary, it would be a hard job for a cyclist to travel along a horizontal track. For the same reason a rider and his horse lean inwards on a sharp turn. Let’s pass on from small to large-scale phenomena. The Earth, on which we live, rotates and so centrifugal force should manifest itself. But where and how? By making all the things on its surface lighter. The closer something is to the Equator, the larger the circle in which it moves and hence it rotates faster, thereby losing more of its weight. If a 1-kg mass were to be brought from one ofthe poles to the Equator and reweighed using a spring balance, the loss in weight would amount to 5 grammes. That, of course, is not very much of a difference, but the heavier a thing, the larger the difference. A locomotive that has come from Stockholm to Rome loses 60 kg, the weight of an adult. A battle ship of 20,000-tonne displacement that has come from the White Sea to the Black Sea will have lost as much as 80 tonnes, the weight of a locomotive! Why does it happen? Because as the globe rotates, it For Young Physicists tries to throw everything off its surface just like the umbrella in our earlier experiment. It would succeed were it not for the terrestrial attraction that pulls everything back to the Earth’s surface. We call this attraction “gravity”. The rotation cannot throw things off the Earth’s surface, but it can make them lighter. The faster the rotation, the more noticeable the reduction in weight. Scientists have calculated that if the Earth rotated 17 times faster, things at the Equator would lose their weight completely to become weightless. And if it rotated yet quicker, making, say, one turn every hour, then the weight lessness would extend to the lands and seas farther away from the Equator. Just imagine things losing their weight. It would mean there would be nothing you could not lift, you would be able to lift locomotives, boulders, cannons and warships as easily as you could a feather. And should you drop them-no danger, they could hurt nobody since they wouldn’t fall down at all, but would float about in mid-air just where you’d let go of them. If, sitting in the cabin of an airship, you wanted to throw something overboard, it wouldn’t drop, but would stay in the air. What a wonder world it would be. So you could jump as high as you’ve never dreamed, higher than sky-scrapers or the mountains. But remember, it would be easy to jump up but diffi¬ cult to return back to ground. Weightless, you’d never come back on your own. There would also be other inconveniences in such a world. You’ve probably realized yourself that everything, whatever its size, would, if not fixed, rise up due to the slightest motion of air and float about. People, animals, cars, carts, ships-everything would move about in the air disorderly, breaking, maiming and destroying. That is what would occur if the Earth rotated sig¬ nificantly faster. Ten Tops The accompanying figures show 10 types of tops. These will enable you to do a number of exciting and instructive experiments. You don’t need any special skill to construct them so you can make them yourself without any help or expense. This is how the tops are made: For Young Physicists 56-57 Figure 21 Figure 22 Figure 23 Figure 24 Figure 25 1. If a button with five holes -comes your way, like the one shown in the figure, then you can easily make it into a top. Push a match with a sharpened end through the central hole, which is the only one needed, wedge it in and then... the top is ready. It will rotate on both the blunt and pointed end, you only need to spin it as usual by twisting the axle between your fingers and dropping the top swiftly on its blunt end. It will spin rocking eccentrically. 2. You could do without a button, a cork is nearly always at hand. Cut a disk out of it, pierce the disk with a match, and you have top No. 2 (Fig. 22). 3. Figure 23 depicts a rather unusual top-a walnut that spins on the pointed end. To turn a suitable nut into a top just drive a match into the other end, the match being used for spinning the top. 4. A better idea is to use a flat wide plug (or the plastic cover of a small can). Heat an iron wire or knitting-needle and burn through the plug along the axis to form a channel for the match. A top like this will spin long and steadily. 5. Figure 24 shows another top: a flat round box pierced by a sharpened match. For the box to fit tightly without sliding along the match, seal the hole with wax. 6. A fancy top you see in Figure 25. Globular buttons with an eye are tied to the edge of a cardboard disk with pieces of string. As the top rotates the buttons are thrown off radially, stretching the strings out taut and graphically demonstrating the action of our old friend, the centrifugal force. 7. The same principle is demonstrated in another way by the top in Figure 26. Some pins are driven into the cork ring of the top with coloured beads threaded onto them so that beads can slide along the pin. As the top spins the beads are pushed away to the pin heads. If the spinning top is illuminated, the pins merge into a solid silvery belt with a coloured fringe of the merged beads. In order to enjoy the illusion spin the top on a smooth plate. 8. A coloured top (Fig. 27). It is fairly laborious to make but the top will reward your efforts by demonstrating an astounding behaviour. Cut a piece of cardboard into a disk, make a hole at the centre to receive a pointed match. Clamp the match on either side of the disk with two cork disks. Now divide the cardboard disk into equal sectors by straight radial lines in the same way a round cake is shared out. For Young Physicists Figure 28 Figure 29 n. Figure 30 Colour the sectors alternately in yellow and blue. What will you see as the top rotates? The disk will appear neither blue nor yellow, but green. The blue and yellow colours merge in your eye to give a new colour, green. You can continue your experiments on colour blending. Prepare a disk with sectors alternately coloured in blue and orange. Now, when the disk is spun it will be white, not yellow (actually it will be light grey, the lighter the purer the paints). In physics two colours that, when blended, give white are called “complementary”. Consequently, our top has shown that blue and orange are complementary. If you have a good set of paints you can try an experiment that was first done 200 years ago by the great English scientist Isaac Newton. Paint the sectors of a disk with the seven colours of the rainbow which are: violet, indigo, blue, green, yellow, orange, and red. When all the seven colours are rotated together they will produce a greyish-white. The experiment will help you to understand that the sunlight is composed of many colours. These experiments can be modified as follows: as the top spins throw a paper ring onto it and the disk will change its colour at once (Fig. 28). 9. The writing top (Fig. 29). Make the top as just described, the only difference being that its axle will now be a soft pencil, not match. Make the top spin on a cardboard sheet placed somewhat at an angle. The top will, as it spins, descend gradually down the inclined cardboard sheet, with the pencil drawing flourishes. These are easy to count and, since each one corresponds to one turn of the top, by watching the top with a clock in hand* you can readily determine the number of revolutions the top makes each second. Clearly, this would be impossible in any other way. A further form of the writing top is depicted in Fig. 30. Find a small lead disk and drill a hole at the centre (lead is soft and drilling it is easy), and a hole on either side of it. Through the centre hole a sharpened stick is passed, and through one of the side holes a piece of fishing-line * By the way, seconds can also be reckoned without a clock just by counting. To do so, you should at first drill yourself a bit to pronounce “one”, “two”, “three”, etc., so that each number takes exactly one second to pronounce. Don’t think that it’s difficult, the practice shouldn’t take more than 10 minutes. 58-59 For Young Physicists (or bristle) is threaded so that it protrudes a bit lower than the end of the top axle. The fishing-line is fixed in with a piece of match. The third hole is left as it is, its only purpose is to balance the disk since otherwise the top won’tspin smoothly. Our writing top is ready, but to experiment with it we need a sooty plate. Hold a plate over a smoky flame until it is covered with a uniform layer of dense soot. Then send the top spinning over the sooty surface. It will slide over the surface and the end of the fishing-line will draw, white on black, an intricate and rather attractive ornament. 10. Our crowning effort is the last rig, the merry-go- round top. However, it is much easier to make that it might seem. The disk and stick here are just as in the Figure 31 earlier coloured top. Into the disk, pins with small flags are stuck symmetrically about the axis, and tiny paper riders are glued in-between the pins. Thus, you have a toy merry-go-round to amuze your younger brothers and sisters. Impact When two boats, trams or croquet balls collide (an incident or move in a game) a physicist would call such an event just “impact”. The impact lasts a split second, but if the objects involved are elastic, which is normally the case, then a lot happens in this instant. In each elastic impact physicists distinguish three phases. In the first phase both colliding objects compress each other at the place of contact. Then comes the second phase when the mutual compression reaches a maximum, the internal counteraction begins in response to the compression and prevents the bodies from compressing further, so balancing the thrusting force. In the third phase the counteraction, seeking to restore the body’s shape deformed during the first phase, pushes the objects apart in opposite directions. The receding For Young Physicists object, as it were, receives its impact back. In fact, when we observe, say, one croquet ball striking another, stationary, ball of the same mass, then the recoil makes the oncoming ball stop and the other ball roll forward with the velocity of the first. It is very interesting to observe a ball striking a number of other balls arranged in a file touching each other. The impact received by the first ball is, as it were, transferred through the file, but all the balls remain at rest and only the outermost one jumps away as it has no adjacent ball to impart the impact to and receive it back. This experiment can be carried out with croquet balls, but it is also a success with draughts or coins. Arrange the draughts in a straight line, it can be a very long one, but the essential condition is that they touch one another. Holding the first draught with a finger strike it on its edge with a wooden ruler, as shown. You will see the last draught jump away, with the rest of the draughts remaining in their places. An Egg in a Glass Circus conjurers sometimes surprise the public by jerking the cloth from a laid table so that everything- plates, glasses, and bottles-remain safely in place. This is no wonder or deceit, it is simply a matter of dexterity acquired by prolonged practice. Such a sleight-of-hand is too difficult for you to attain but on a smaller scale a similar trick is no problem. Place a glass half-filled with water on a table and cover it with a postcard (or half of it). Further, borrow a man’s wide ring and a hard-boiled egg. Put the ring on the top of the card, and stand the egg on the ring. It possible to jerk the card away so that the egg doesn’t roll down onto the table? At first sight, it may seem as difficult as jerking the 60-61 For Young Physicists table-cloth from under the table things. But a good snap with a finger on the edge of the card should do the trick. The card flies away and the egg... plunges with the ring safely into the water. The water cushions the blow and the shell remains intact. With some experience, you could try the trick with a raw egg. This small wonder is explained by the fact that during the fleeting moment of the impact the egg doesn’t receive any observable speed but the postcard that was struck has time to slip out. Having lost its support, the egg drops into the glass. If the experiment is not at first a success, first practice an easier experiment in the same vein. Place half a postcard on the palm of your hand and a heavy coin on top of it. Now snap the card from under the coin. The card will fly away but the coin will stay. Unusual Breakage Conjurers sometimes perform an elegant trick that seems amazing and unusual, though it can be easily explained. A longish stick is suspended on two paper rings. One of the rings is suspended from a razor blade, the other, from a clay pipe. The conjurer takes another stick and strikes the first one with all his strength. What happens? The suspended stick breaks but the paper rings and the pipe remain absolutely intact! The trick can be accounted for in much the same way as the previous one. The impact was so fast that it allowed no time for the suspended stick’s ends and the paper rings to move. Only the part of the stick that is directly subjected to the impact moves with the result that the stick breaks. The secret is thus that the impact was very fast and sharp. A slow, sluggish impact will not break the stick but will break the rings instead. The most adroit conjurers even contrive to break a stick supported by the edges of two thin glasses leaving the glasses intact. I do not tell you this, of course, to encourage you to do such tricks. You’ll have to content yourself with a more modest form of them. Put two pencils on the edge of a low table or bench so that part of them overhang and place a thin, long stick on the over¬ hanging ends. A strong, sharp stroke with the edge of a ruler at the middle of the stick would break it in two, but the pencils would remain in their places. For Young Physicists Figure 35 Now it should be clear to you why it is difficult to crack a nut by the strong pressure of a palm, but the stroke of a fist does the job easily. When you hit it, the impact has no time to propagate along the flesh of your fist so that your soft muscles do not yield under the upthrust of the nut and act as a solid. For the same reason a bullet makes a small round hole in the window-pane, but a small stone traveling at a far slower speed breaks the pane. A slower push makes the window frame turn on its hinges, something neither the bullet nor the stone can make it do. Finally, one more example of the phenomenon is being able to cut a stem of grass by a stroke of a cane. By slowly moving the cane you can’t cut a stem, you only bend it. By striking it with all your strength you will cut it, if, of course, the stem is not too thick. Here, as in our earlier cases, the cane moves too fast for the impact to be transferred to the whole of the stem. It will only concentrate in a small section that will bear all the consequences. Just Like a Submarine A fresh egg will sink in water, a fact known to every experienced housewife. If she wants to find out whether an egg is fresh, she tests it in exactly this way. If an egg sinks, it is fresh; and if it floats, it is not suitable for eating. A physicist infers from this observation that a fresh egg is heavier than the same volume of fresh water. I say “fresh water” because impure (e.g. salt) water weighs more. It is possible to prepare such a strong solution of salt that an egg will be lighter than the amount of brine displaced by it. Then, following the principle of floating discovered in olden days by Archimedes, even the freshest of eggs will float in the solution. For Young Physicists Use your knowledge in the following instructive experiment. Try to make an egg neither sink nor float, but hang in the bulk of a liquid. A physicist would say that the egg is “suspended”. You’ll need a water solution of salt that is so strong that an egg submerged in it displaces exactly its own weight in the brine. The brine is prepared by the trial-and-error method: by pouring in some water if the egg surfaces andadding some stronger brine if it sinks. If you’ve got patience, you’ll eventually end up with a brine in which the submerged egg neither surfaces nor sinks, but is at rest within the liquid. This state is characteristic of a submarine. It can stay under water without touching the ground only when it weighs exactly as much as the water it displaces. For this weight to be reached, submarines let water from the outside into a special container; when the submarine surfaces the water is pushed out. A dirigible-not an aeroplane but just a dirigi¬ ble-floats in the air for the very same reason: just like the egg in the brine it diplaces precisely as many tonnes of air as it weighs. Floating Needle Is it possible to make a needle float on the surface of water like a straw? It would seem impossible: a solid piece of steel, although it’s small, would be bound to sink. Many people think this way and if you are among the many, the following experiment will make you change your mind. Get a conventional (but not too thick) sewing needle, smear it slightly with oil or fat and place it carefully on the surface of the water in a bowl, pail, or glass. To your surprise, the needle will not go down, but will stay on the surface. Why doesn’t it sink, however? After all, steel is heavier than water? Certainly, it is seven to eight times as heavy as water, if it were under the water it wouldn’t be able to surface like a match. But our needle doesn’t submerge. To find a clue, look closely at the surface of the water near the floating needle. You’ll see that near the needle the surface forms sort of a valley at the bottom of which lies our needle. The surface curvature is caused by the oil-smeared needle being not wetted by the water. You may have For Young Physicists noticed that when your hands are oily, water doesn’t wet the skin. The feathers of water birds are always covered with oil exuded by a gland, which is why water doesn’t wet feathers (“like water off a duck’s back”). And again this is the reason why without soap, which dissolves the oil film and removes it from the skin, you cannot wash your oily hands even by hot water. The needle with oil on it is not wetted by water either and lies at the bottom of a concavity supported by the water “film” created by surface tension. The film seeks to straighten and so pushes the needle out of the water, preventing it from sinking. As our hands are always somewhat oily, if you handle a needle it will be covered by a thin layer of oil. Therefore, it is possible to make the needle float without specially covering it with oil-you’ll only have to place it extremely carefully on some water. This can be made as follows: place the needle on a piece of tissue-paper, then gradually, by bending down the edges of the paper with another needle, submerge the paper. The paper will descend to the bottom and the needle will stay on the surface. Now if you came across a pondskater scuttling about the water surface, you won’t be puzzled by it. You’ll guess that the insect’s legs are covered with oil and are not wetted by the water and that surface tension supports the insect on the surface. Diving bell This simple experiment will require a basin, but a deep, wide can would be more convenient. Besides, we’ll need a tall glass (or a big goblet). This’ll be our diving bell, and the basin with water will be our “sea” or “lake”. There is hardly a simpler experiment. You just hold the glass upside down, push it down to the bottom of the basin holding it in your hand (for the water not to push it out). As you do so you’ll see that the water doesn’t find its way into the glass-the air doesn’t let it in. To make the performance more dramatic, put something easily soaked, e.g. a lump of sugar, under your “bell”. For this purpose, place a cork disk with a lump of sugar on it on the water and cover it by the glass. Now push the glass into the water. The sugar will appear to be below the water surface, but will remain dry, as the water doesn’t get under the glass. You can perform the experiment with a glass funnel. 64-65 Figure 39 For Young Physicists if you push it into the water, its wider end down and its narrow end covered tightly with a finger. The water again doesn’t get inside the funnel, but once you remove your finger from the hole, thereby letting the air out of the funnel, the water will promptly rise into the funnel to reach the level of the surrounding water. You see that air is not “nothing”, as some think, it occupies space and doesn’t let in other things if it has nowhere to go. Besides, these experiments should graphically illustrate the way in which people can stay and work under water in a diving bell or inside wide tubes that are known as “caissons”. Water won’t get into the bell, or caisson, for the same reason as it can’t get into the glass in our experiment. Why Doesn't It Pour Out? The following experiment is one of the easiest to carry out, it was one of the first experiments I performed when I was a boy. Fill a glass with water, cover it with a postcard or a sheet of paper and, holding the card slightly with your fingers, turn the glass upside down. You can now take away your hand, the card won’t drop and the water won’t pour out if only the card is strictly horizontal. You can safely carry the glass about in this position, perhaps even more comfortably than usually since as the water won’t spill over. As the occasion serves, you can astound your friends (if asked to bring some water to drink) by bringing water in a glass upside down. What then keeps the card from falling, i.e. what overcomes the weight of the water column? The pressure of air! It exerts a force on the outside of the card that can be calculated to be much greater than the weight of the water, i.e. 200 grammes. The person who showed me the trick for the first time also drew my attention to the fact that the water must fill the glass completely for the trick to be a success. If it only occupies a part of the glass, the rest of the glass being filled by air, the trial may fail because the air inside the glass would press on the card balancing off the pressure of the outside air with the result that it might fall down. When I was told this, I set out at once to try it with a glass that wasn’t fully filled in order to see for myself of the card would drop. Just imagine my astonishment 5-621 For Young Physicists when I saw that in that case too, it didn’t fall! Having repeated the experiment several times, I made sure that the card held in place as securely as with the full glass. This has taught me a good lesson about how the facts of nature should be perceived. The highest authority in natural science must be experiment. Every theory, however plausible it might seem, must be tested by experiment. “Test and retest” was the motto of the early naturalists (Florentine academicians) in the 17th century, it is still true for 20th century physicists. And should a test of a theory indicate that experiment doesn’t bear it out, one should dig for the clues to the failure of the theory. In our case we can easily find a weak point in the reasoning that once had seemed convincing. If we carefully turn back a corner of the card covering the overturned, partially filled glass, we’ll see an air bubble come up through the water. What is it indicative of? Obviously the air in the glass was slightly rarefied, otherwise the outside air wouldn’t rush into the space above the water. This explains the trick: although some air remained in the glass, it was slightly rarefied, and hence exerted less pressure. Clearly, when we turn the glass over, the water, as it goes down, forces some of the air out of the glass. The remaining air, which now fills up the same space, becomes rarefied and its pressure becomes weaker. You see that even simplest
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