-Ti* <$cuUo^($J,) 7u^ 'fa+^'t V ~>c ->c x. >c ^ ^ I I Page numbering is irregular. Text is complete. THE BOOK OF PHILOSOPHICAL EXPERIMENTS. ILLUSTRATING THE PRINCIPAL FACTS AND CURIOUS PHENOMENA OF ELECTRICITY, GALVANISM, MAGNETISM, OPTICS, CHEMISTRY, HEAT, ETC. WITH INTRODUCTORY OBSERVATIONS ON EACH SCIENCE, AND UPWARDS OF 300 " BY J I EXPERIMENTS. .S.DALTON TO MY KIND FRIEND, JOHN ALLISTON, ESQ., One of the Directors of the Provincial Bank of Ireland, a Governor of Ckritt's Hospital, #c, ft. I MOST RESPECTFULLY DEDICATE THIS LITTLE VOLUME, AS A MARK OP MY HIGH RESPECT AND ESTEEM FOR HIS CHARACTER, A\D AS A SLIGHT REMEMBRANCE OF HIS KINDNESS TO THE AUTHOR. $&- This work has two objects in view. First, to provide young persons with the means of obtaining a knowledge of some of the most important phenomena of nature, and the applications of science to purposes of utility ; and secondly, to furnish them with an almost inexhaustible fund of amusement for winter evenings, and other occasions, when ex- ercises in the open air are obliged to make way for in-door recreations. There is no person, however illiterate, but experiences some degree of pleasure on witnessing the performance of scien- tific experiments ; and young persons are more particularly delighted with them. It isjioped, therefore, that the volume now offered to their notice will be accepted with pleasure, as it will enable thein, not only to understand many curious facts in nature, but will instruct them also how to perform a great variety of beautiful experiments themselves, without risk or danger. For conveying instruction in the sciences, experiment is superior to every other method. A person who performs an ex- periment, and thoroughly understands the nature of it, will hardly ever forget the principle it illustrates ; because the fact will be impressed upon the memory in the strongest manner. Young persons may learn, by experiment, what cannot be taught them by mere description ; and the natural curiosity of youth leads them to desire earnestly to become acquainted with the principal laws of nature. No amusement is more gratifying to them than to be engaged in this way ; and hence- tha pleasure with which they peruse such works as the " Endless Amusements," and others of a similar description. These works, however, have been generally deficient in an important particular : they do not explain the causes of the effects they describe, and they are, consequently, much less interesting and instructive than they might be made. This fault has been remedied in the present work ; and such directions are given, that no possible danger can be incurred in per- forming the experiments. Some elementary books on science contain a number of scientific illustrations, that cannot be performed without considerable risk, even by persons who are familiar with the subject: what must be the danger, then, when ignorant persons attempt to perform them, without having received the least caution ? Serious accidents are frequent- ly the result. In this work, experiments that cannot be performed without danger are omitted, and cautionary remarks are tiven whenever necessary, in order to prevent the. possibility of accident. As the " Book of Experiments" is intended chiefly for the amusement and instruction of young persons, it will not be expected to contain any elaborate views of science. It has been the endeavor of the Editor to collect and arrange only such experiments as might easily be understood, and such as explain, in a pleasing manner, the principles of many of the plienom ena of daily life. Some of the illustrations are derived from sources not easily accessible ; others are those which the most eminent scientific lecturers of the present day are in the habit of employing ; and the remainder, it is believed, have never be- fore been published. The whole ore simple and striking, and will, it is hoped, have the effect of stimulating the minds of those who practice them to become still better acquainted with " divine philosophy ;" and, by observing the beautiful har- mony that pervades the whole material universe, " Look through nature up to Nature's God." ELECTRICITY. I ntrodnctiou to the science—Theor.es of electricity—Conduc- tors and non-conductors—Ri;> n transmission of electri- city—Galvanism—Magnetism—Description of an electrical machine—a Leyden jar—How to make cheap electrical machines of paper—Ditto of glass—How an electrical machine acts. 1. The word electricity is used to express the cause of a great variety of phenomena^ which take place when certain substances are gabbed against each other; and it is found, by experi- ment, to be identical with lightning. It is sup. posed to be an extremely subtle fluid, which near- ly all bodies are capable of producing under cer- tain circumstances. It is commonly obtained. for the purpose of experiment, by the friction oc. casioned by rubbing glass with silk. An arrange, ment of these substances, in a peculiar manner, constitutes an electrical machine, by which large ^13 40 Philosophical Experiments. quantities of the electric fluid may be obtained. When thus accumulated, it is found to possess the power of passing through some substances with extreme facility, which are, therefore, term- ed good conductors; while other bodies retain it entirely, or very much impede its progress ; such substances are termed non-conductors, and are usually employed for the purpose of obtaining electricity by friction, as before mentioned. The electric fluid obtained by the electrical machine, and that obtained from the clouds, which is light- ning, are identical in their properties; and the electricity procured by either method is found to cause attraction and repulsion between bodies ; to be capable of decomposing water and other chemical compounds, into their elements; and when passed through living bodies, in considera- ble quantities, of destroying life. It travels with an inconceivable velocity, like light, through good conductors, passing only along their sur- faces; and it is, undoubtedly, the cause of many vital and chemical phenomena, as well as being closely identified with galvanism and magnetism. It is wonderful to trunk that " the forked light- ning," which, at all times, presents an appearance that cannot be contemplated without some de- gree of awe, and which, occasionally, is terrific, is identical in all respects, except that it is more powerful, with the electric spark that may be ob- tained from a common sheet of paper, as describ- ed hereafter. Yet such is undoubtedly the case; for Franklin, and other philosophers since his time, have drawn lightning from the clouds by means of silk kites, and found it resemble, in ev- ery respect, that which they obtained from an electrical machine. Some philosophers have supposed that there are two kinds of electricity, which they have termed resinous, because it is produced abundantly from resinous substances, and vitreous, because procured from glass. Dr. Franklin supposed that there were not two kinds of electricity, but that it existed in two different conditions, which he termed positive and negative. These distinc- tions will be best explained by the experiments: it is only necessary now to mention that, which- ever theory of electricity is preferred, the same facts are explicable by both of them, since sub- stances, in a similarly electrical condition, al- ways repel each other, and when in opposite states, they attract each other. This is illustra- ted by experiment 18. 3. Electricity is not produced by the friction of two portions of one substance, but when dif- ferent substances are rubbed together, the electric fluid is obtained ; and, if the bodies employed are bad conductors, it accumulates, according to the time the friction is continued; while, if the sub- stances are good conductors, it passes away as quickly as it is obtained, and the usual phenom- ena does not take place. The worst conductors are, therefore, the best substances from which electricity can be pro- duced ; amber, wax, glass, silk, hair, and dried wood, are a few of these. Steam and vapor, smoke, living animals, vegetables, water, and the different metals, are good conductors; and little or no electricity can therefore be procured from them, since they conduct it away as quickly as it is obtained. Bodies having points on their sur- face readily give off, as well as receive, electri- city ; and are, therefore, unfit to be used for the purpose of retaining it. Lightning conductors—the long, pointed rods of iron that are placed against high chimneys and buildings, in order to prevent their being struck by the electric fluid—are examples of the manner in wliich a knowledge of the facts just related may be applied to useful purposes. Iron, being one of the metals, is a good conductor j and when, therefore, a cloud, charged with elec- tricity, passes near it, it establishes a communica- tion between the earth and the cloud, and thus prevents the serious consequences which ensue when the electric fluid endeavors to find a passage through a bad conductor. As just mentioned, living vegetables are good conductors; and it therefore frequently happens that a cloud dischar- ges itself by means of a tree; but in passing through it, the vitality of the tree is destroyed, in the same way that animals may be killed by hav- ing a powerful shock passed through them. It is extremely dangerous for persons to take shelter under a tree during a thunder storm; because, if the tree be struck by lightning, it may proba- bly pass through their bodies in descending to the earth, as they are as good conductors as the tree. 4. The rapidity with which lightning travels is inconceivable; and it is the same with the electric fluid procured artificially. A wire has been attached to a portion of an electrical batte- ry, and after being extended for two or three miles, in folds, the other end has been made to communicate with an explosive compound, in or- der to ascertain how much time would expire be- tween the discharge from the conductor and the explosion. In every case they appeared to take place at the same moment; and all other experi- ments that have been performed for a similar pur- pose, have tended to prove that the passage of the electric fluid is instantaneous. The principal phenomena of electricity will be found described and illustrated in the following experiments; among them, also, are a few in gal- vanism and magnetism, wliich must, therefore, be briefly alluded to. 5. Galvanism is so termed from the nature of the person who first noticed some of the re- markable effects it is capable of producing. Gal- vani found, that when he brought the point of a knife in contact with the nerve of a frog, a por- tion of whose body was in contact with the prime conductor of an electrical machine, that the ani- mal was violently convulsed; and following up these experiments, by the assistance of a friend, he constructed what is termed the galvanic batte. ry. This consists of a number of plates of zinc and copper, placed side by side, and immersed in a dilute acid, which, acting on the surface of the metals, produce a current of galvanism, that, passing off at each end by means of two wires, may be made to form a circuit through any sub- stance. All the metals, when exposed to gal- vanic influence in this way, become liquid, and compound bodies are decomposed; the elements in a positive state of electricity passing off to one pole, and those in a negative state to the other. Illustrations of these facts will be found in the ensuing pages, where a description is like- wise given of the best means of constructing a Philosophical Experiments. 41 galvanic battery, and a voltaic pile, and how to illustrate their effects. 6. Magnetism is the term used to express the property of the loadstone, with Vhich most per- sons are familiar. It is well known that the load- stone will attract iron and steel, and that the lat- ter, by being rubbed on the loadstone, becomes a magnet; one end of which will always point to the north pole, and the other to the south. The advantages that inin has derived from this circum. Ftance in being able, at all times, to determine with exactness his situation at sea, when sur- rounded on all sides with an apparently bound- less ocean, arc too well known to require com- ment. It has only quite lately, however, been deter. mined that the direction of the magnet is occa- sioned by currents of electricity, which arc con- stantly passing across the earth from west to east, and that the magnet is, therefore, always at right angles to this current. That this is the case, however, is clearly proved by experiment 79. It is also capable of proof that magnetism is a mod- ification of electricity. By experiment 77, it will be seen that, by passing a current of elcctri- city round a steel bar, it becomes a magnet, pos- sessing all the properties of one formed by fric- tion on a loadstone; and electro-magnetic ma- chines may now be seen in the opticians' shops, by wliich the electric spark can be procured from magnets themselves. SIMPLE ELECTRICAL MACHINES. 7. A few of the more important effects of elec- tricity, can be exhibited without the assistance of an electrical machine ; yet it is so very expensive a piece of apparatus, and so liable to accident, that fe\v*of our readers will probably be induced to purchase one from a mathematical instrument maker. They may occasionally be met with cheap, second-hand; but as few pereons have the opportunity of procuring them in this way, wc have described, in the following pages, several methods by which, with a little ingenuity, and at a trifling expense, any one may make a good elec- trical machine for himself. The principal parts of a good machine are, a cylinder, or a plate of glass, from which electri- city is to be obtained by causing it to rub against a piece of silk, covered with an amalgam; the method of preparing which will be described here- after. As the electricity accumulates, it is passed to a hollow cylinder of metal, supported on a glass leg, so that the electricity cannot escape from it, which is called the prime conductor; and from this reservoir, such quantities of the electric fluid as may be required, can be obtained. It is ne- cessary that the rubbing surfaces should be con- nected, by a chain, with the ground, or other- wise : in a short time, the silk is incapable of giving off anymore electricity, being, in fact, in- sulated by the dry wood of the table on which it may be standing, just as the prime conductor is by its glass supporter. 8. A Leyden jar is used to contain electricity, so that when many of them, of large size, are at- tached together, a great quantity of the fluid may be accumulated, and then the most powerful ef- fects can be produced. The jar is formed of lass, and is coated, inside and out, with tin foil, y which the electricity is diffused over both sur- faces. A description of the best method of mak- ing one cheaply wdl be found in a subsequent page. 9. It has been previously mentioned, that not only glass, but all substances that are bad con- ductors of electricity, are the best from which to obtain the electric fluid. Accordingly, brown paper, being a non-conductor, may be used for the purpose; and the following is a simple plan for making an electric machine with it:—Take a circular piece of wood, about one inch thick, and of convenient diameter, and paste over it a sheet of brown paper, cutting the edges even; then paste a strip all round the edge of the cir- cle, and when quite dry, paste on another coat- ing of the brown paper in the same manner ; then cut a square hole in the centre, and pass through it the axle, wliich mount on two pieces of wood as pillars. A piece of wood, staple-shaped, and covered with silk, or woolen cloth, will do for the rubber ; and a cylindrical piece of wood, like a rolling-pin, with rounded ends, covered with tin foil, and mounted on a wine bottle, serves for the prime conductor ; three or four wires or needles, being inserted in the wood, to collect the elec- tricity from the two sides and edges of the wheel. 10. A glass electrical machine, of the cylin- drical form, may be made at a very trifling ex- pense. The following is an extremely ingenious method of constructing one from the most simple materials:— First, drill a sufficient hole through the bottom of a common wine bottle, opposite the mouth ; or take off the bottom, by igniting a piece of worsted tied round it dipped in turpentine, which will do this. Through this hole and the mouth, pass a spindle, as represented in the engraving (b, c,) v Cfjm'T:SS^v::'J"*°gsM||| ,w, (i, "rc The end of b should be squared, to fix a handle on, and the spindle should be fixed firmly in the bottle. The bottle is then to be fixed in a frame (as represented at page 42,) in the following man- ner :—the end of the spindle c passes through a hole, the diameter of which is the same as that of the spindle in the upright d, and the end b slides down the grove in the other upright, f, the bottom of which is the same hight as the hole in the upright c, so as to keep the bottle in a hori- zontal position ; the spindle is kept from starting up by passing a pin through the upright, in the direction of the line a. Next, make a cushion of wash leather, stuffed with wool, and fasten it with glue on the top of a frame, f, as S^&f f represented in the annexed cut. This (T^,, - frame is to be of such a hight, that k, the cushion shall press against the 'jy , side of the bottle; and a piece of-,f|i..Ui black silk (which, for the sake of* | clearness is omitted in this engraving, &''[.. j but is marked a, in the one at page I *??, '^_j 42,) i6 to be sewn on the top of the L^J cushion, and hang over the bottle, as represented in page 42. The method of keeping this cushion 42 Philosophical Experiments. a d pressing against the bottle will be better understood by reference to the following figure, which is a plan of the board, k, in which the up- rights are fixed; a and b are the places for the up- rights; c and d are the holes in which the ends .'Xj of the cushion frame are put. A long wedge (see^ cut on the right) is put in the hole e, and another wedge is then put be- tween the cushion frame and the upright wedge. This is better explained by the following engra- ving, where f, is a side view of the cushion from l, the upright wedge, and m, the wedge which is put be- tween the cushion frame and the up- right wedge. The cushion should be smeared with an amalgam, formed by melting together, in the bowl of a tobacco-pipe, or in a crucible, one part of tin, with two of zinc; to which, while fluid, ssix parts of mercury should be added, and stirred about till cold, when it is to be reduced to fine powder in a mortar, and mixed with a suffi- cient quantity of lard to form a paste. If this cannot, however, be easily obtained, a little quick- silver, scraped from the back of a broken piece of looking-glass, and mixed with tallow, may be used instead. When this is done, the machine will be complete, and its appearance is represented in the annexed engraving. The letters refer to the part before described. If the cushion be pressed A C against the bottle with the hand, it will cause the machine to work better; and before it is used, it should be held before the fire for a minute or two, in order that the bottle may be perfectly dry, as moisture conducts the electricity away. This is the reason why many experiments, which suc- ceed on a clear, dry day, fail when the atmos- phere is filled with moisture. A prime conductor for the above machine may be made thus :—at right angles to one end of a cylinder of wood, about two inches and a half in diameter, and six inches long, fix a small wooden cylinder, about three quarters of an inch in di- ameter, and three inches long, rounded at both ends ; the other end of the larger cylinder is also to be rounded. Cover the whole with tin foil, and mount it on a stand on a glass rod. When used, it is to be placed with the cross-piece in a line even with, and about half an inch from the bottle ; and it should be of such a hight as just to come below the silk apron. When it is wished to charge a Leyden jar, it is to be placed at the round end of the conductor. 11. The mode in wliich the electrical machine just described, and others, act, will be easily un- derstood from the following description:—The friction of the cushion against the glass cylinder (bottle,) produces a transfer of the electnc fluid from the cushion to the bottle; that is, the cushion becomes negatively, and the glass positively elcc. trifled. The fluid which thus adheres to the glass, is carried round by the revolution of the cylinder, and its escape is at first prevented by the silk flap which covers the cylinder, untd it comes to the immediate vicinity of the part that projects from the prime conductor ; and which, being placed at a small distance from the cylinder, absorbs nearly all the electricity as it passes near it, and trans- fers it to the prime conductor. Positive electri. city is thus accumulated in the prime conductor, while the cushion, being deprived of its electricity, is negatively electified. 12. An electrical machine may be made, with- out the trouble of forming a hole through the bot- tom of a bottle, by attending to the following directions :—The rubber is to be glued to a piece of wood, which is then to be inserted into the neck of a small bottle, as shown by a in the en- graving annexed, and secured by sealing-wax. A piece of leather should then be tied tightly near the bottom of the bottle, at back, as at b, the end of which is to be nailed to the stand to secure it, as a hinge. In front of the bottle is then to be tied a piece of Indian rubber, the end of which is also to be made fast to the stand, as at c, so that when the rubber is , pressing against the cyl-1 inder, the elasticity of the Indian rubber per- mits the cushion to yield to the inequalities of the cylinder,andthe pressure is always nearly equal. d, represents the cylin- der ; and above a, is a knob (a piece of bent wire may be used instead,) to receive the spark from. If the cylinder is made of a green glass bottle, the positive spark will be given out by the rubber, and the negative by the conductor; but if of white glass, the con- trary will take place. 13. One of the greatest difficulties in con- structing the machine first described, is making a hole in the bottom of the bottle, whick is to serve as a cylinder. This difficulty may be avoided by fixing a piece of wood in the centre of the concavity at the bottom of the bottj^ while melted sealing-wax is dropped in untiWthe stick is well surrounded, as in the accompanying figure. On the wax, cooling, the stick will remain quite firm. Care should be taken to fix it exactly opposite the spindle that is to be fixed in the neck of the bottle. Thus, with a little ingenuity, any one who wishes to study the science of electricity may easily make himself a cheap machine for the pure pose; and by doing so, he will have the addi- tional advantage of perfectly understanding th- different parts of which it is formed. -■ Philosophical Experiments. 43 EXPERIMENTS. Electrical attraction-Repulsion-Electrified ribbons-De Luc's column—Identity of the electric fluid—Positive and nega- tive electricity—The discharging rod—Working power of electricity—Electricity from a cat's back—Electrome- ters—To draw sparks of fire from the body—To ignite ether by the touch—Electrified head of hair—An elec- trified kiss—The ringing belU—The jumping balls—The The. sportsman—Luminous figures by electricity—To im- itate the sound of thunder—Imitation thunder clouds— The cause of thunder—Place of safety in a thunder storm —Electrified sheet of paper—The electrophorus—To charge the. electrophone—Description of the electric spark. THE LEYDEN JAR. 14. Tuis is one of the most useful pieces of electrical apparatus. It is employed for the pur- pose of containing a quantity of electricity, which may thus be applied to any substance. It consists of a glass jar, coated, both inside and out, nearly to the top, with tin foil, by which the electri- city is equally distributed. A krTob rises through a wooden top, communicating with the inside of a jar. When it is wished to change it, this knob is applied to the prime conductor of an electrical machine in ac- tion, and the jar will remain charged till a con- nection is made, by some good conductor, be- tween the knob and the outside tin foil. 15. A Leyden jar may be made out of a com- mon wine bottle, with about three inches of iron filings in it, ftncffilled to the shoulder with water. Coat it on the outside with tin foil, and pass a wire througli the cork, one end reaching the iron filings, and the other terminating in a brass knob. By this means, the necessity of coating the in- side of the jar with tin foil, a work of much diffi- culty, may be avoided. ELECTRICAL ATTRACTION. 16. If a piece of amber be rubbed on a coat- sleeve for a short time, or on a piece of silk, which is preferable, it becomes electrified, and will attract light substances, &c. It was the discovery of this peculiar property of amber that first directed the attention of philosophers to elec- trical phenomena. i7. If a piece of sealing-wax be rubbed in a similar manner to amber, it wall exhibit the same properties. \ mECTRICAL REnXsiBN. 18. Electrify a smooth glass tube with a silk rubber, and hold a small feather at a short dis- tance from it; the feather will immediately fly to the tube, and adhere to it for a short time, and then fly off; and the tube can never be brought close to the feather till it has touched the side of the room, or some other body that communicates with the ground. If, therefore, the operator take care to keep the tube constantly between the fea- ther and the side of the room, he may drive it round to all parts, without touching it; and the same side of the feather will be constantly oppo- sed to the tube. 19. If, while the feather is flying before the smooth tube, an excited rough tube, or a stick of sealing wax, be presented to it, it will fly contin- ually from the wax, or from one tube to the other, till the electricity of both is discharged. This was one of the first, and is one of the most com- mon experiments in electricity: it is, however, very entertaining, and well exemplifies electrical attraction and repulsion. 20. If the feathers be attached by threads of silk, the experiments may be performed as repre- sented below, where the left-hand figure repre- sents the pith ball attracted by the glass tube, and the right-hand figure the same ball, when charged with electricity, and repelled by the tube. ELECTRIFIED RIBBONS. 21. If a white and a black ribbon, about two or three feet long, and perfectly dry, be applied to each other by their smooth surfaces, and then drawn frequently between the finger and thumb, so as to rub against each other, they will be found to adhere together; and if pulled asunder at one end, will rush together with great quick- ness. While united, they exhibit no sign of elec- tricity, because the operation of the one is just the reverse of that of the other, and their power is neutralized. If completely separated, how- ever, each will manifest a strong electrical pow- er ; the one attracting those bodies which the other repels. One is positively electrified, the other negatively. DE LUC'S COLUMN. 22. The nearest approach to a perpetual mo- tion, by means of apparatus, is represented in the following figure, known as De Luc's column. It consists of a glass tube, closed at each end by a brass knob, and containing a number of pieces of Dutch leaf, with paper placed between them. By this means electricity is produced, and may be made to attract the pith ball, b, which Is suspend- ed by a silk thread between the column and c, a piece of wood, cover- ed with tin foil, com- municating by a chain with the ground. Af- ter the ball has be- come charged by con- tact with the column, it is repelled, and then flies to the tin-foil con- ductor, where it parts with its excess of elec- tricity, and becomes negative, returning to its perpendicular posi- tion, to be again at- tracted and repelled, as before. By this means the ball will continue in action as long as any electricity is generated, and this may continue for years. 44 Philosophical Experiments. ■*r^ BODIES SIMILARLY ELECTRIFIED REPEL EACH OTHER. 23. If two pith balls be suspended by pieces of silk thread, and electrified, by being touched with excited sealing-wax, or the flannel with which it has been rubbed, the balls will then fly apart from each other; but if one of them be touched with the wax and the other with the flan- nel, they will then mutually attract each other, and adhere together. This experiment illustrates, exceedingly well, one of the principal laws of electricity mentioned in the Introduction ; name- ly, that bodies similarly electrified repel each other, but that when dissimilarly electrified, they attract each other. IDENTITY OF THE ELECTRIC FLUID. If one of the pith balls mentioned in the last ex- periment be electrified with sealing-wax that has been rubbed with flannel, and the other ball by silk rub- bed with glass, these balls will repel each other (as seen in the figure) which proves that the electricity of the silk is the same as that of the sealing-wax; both substances being non- conductors, and, conse- quently, electrics. TO SHOW POSITIVE AND NEGATIVE ELECTRICITY. 25. To show what Franklin termed " positive and negative electricity," and Du- fay, " resinous and vitreous elec- tricity, and that the one is produ- ced from a conductor, and the other from a non-conductor, let one of two balls be electrified by sealing-wax, and the other by glass ; they will then mutually attract each other, showing that they are oppositely electri6cd. THE DISCHARGING ROD. 26. When a Leyden jar is charged with elec- tricity, the inside and the outside are in different states. An equilibrium may be restored, by ap- plying the thumb to the outside, and the fore-fin- ger to the knob communicating with the inside, when the charge will pass through the body, and occasion a shock. As this is sometimes unplea- sant, and when very powerful, even dangerous, the annexed (J^ fd piece of apparatus is used to dis- charge the jar. a, is a glass han- dle ; c c, two balls placed upon two wires, d d, which should be upon a hinge at b, so that they may be be opened wide, if neces- sary. For cheapness, the dis- charger may be merely a piece of bent wire, with a handle of dry wood, wliich is a non-conductor, like glass. When a jar is to be discharged, place one knob on the outside of it, and the other on the knob at the top. Be sure and touch the outside first; for if the knob on the jar is touched first, a severe shock will some- times be given to the experimenter. WORKING POWER OF ELECTRICITY. 27. Electricity may be made to give motion to bodies in the following way :—a, is a wooden board, into which are fixed four glass pillars, b b b b ; the two which stand opposite d, arc to be shorter than those placed at the back of the board; from the top of these stretch fine wires, c c ; at D have a chain attached to your conduct- or ; place on the wire a wheel made of four pieces of wire,, two to be bent round at the ends; fix them in pieces of wood, f ; the other two to ter- minate in a point, and to be fixed in the piece of wood the contrary way to the others; the points to be bent, the one up and the other down, as seen in the engraving. The electricity passes from the prime conductor up the chain at d, over the chains b, up the wire c, on to the wheel, and off at the points, wliich causes it to turn round, and wind itself up the inclined plane. Electricity flies off very quickly from points ; indeed, a can- die may sometimes be blown out from a sharp point on the prime conductor, when charged. 28. A rotary motion may be obtained by the instrument represented in the an- nexed cut. a, is a wire, to-be pla- ced on the conductor of an elec- trical machine ; and the four wires, bbbb, are to be fixed on the top, and bent so as to turn freely on -g, their axis at c. When the ma- chine is put in action, the electri- city flies off from the points, and by the re-action of the air, the wires are forced quickly round. ELECTRICITY FROM A CAT'S BACK. 29. Hair, as previously mentioned, is a non- conductor, and, therefore, may be employed to ob- tain electricity from. Some amusing experiments may be performed with a living cat, by making the hair on her back act as a portion of an elec- trical machine. f Make friends with Pussey—if a black one, so much the better—aAl warm her back well by the fire ; put her
s—Changes of the kaleidoscope.
VELOCITY OF JLIGHT.
G17. Light travels witb the amazing velocity
of 192,000 miles in a second of time; so that it
has been pleasingly remarked, that during a sin-
gle vibration of a commou clock pendulum, it
would go from London to Edinburgh, and back,
200 times although the distance between these
places is 4°^ miles. It may be interesting to
know h"»v philosophers have been able to deter-
mine, with such certainty, that light really travels
with this amazing velocity; for the fact is known
as certainly as any phenomenon in nature. The
method adopted was the following:—The eclipses
of the satellites or moons of the planet Jupiter
had been carefully observed for some time, and a
rule was obtained, which foretold the instants, in
all future time, when the satellites were to glide into
he shadow of the planet, and disappear, or again
to emerge into view. Now it was found that
€6 Philosophical Experiments.
these appearances took place sixteen minutes and
a half sooner when Jupiter was near the earth, or
on the same side of the sun with the earth, than
when it was on the other side; that is to say,
more distant from the earth by one diameter of
the earth's orbit, or path in the heavens which
it takes in revolving round the sun, and at all in-
termediate stations, the difference diminished from
the sixteen minutes and a half, in exact propor-
tion to the less distance from the earth. This
proves, then, that light takes sixteen minutes and
a half to travel across the earth's orbit, and eight
minutes and a quarter for half that distance, or
to come to us from the sun. This being its amazing
velocity, it may, for all useful purposes on the
earth, be regarded as passing between bodies in-
stantaneously ; and it is for this reason that we
perceive the flash from a gun at a distance, for a
perceptible time, before we hear the report, and
why we may count several seconds between the
appearance of a flash of lightning, and hearing
the thunder which follows.
LIGHT TRAVEL3 I.N STRAIGHT LINE8.
218. To prove that fight proceeds from lumin-
ous bodies, in straight lines (see introduction,)
procure a straight flexible tube, and look through
it at any object, which will then be distinctly
visible. If, however, one end of the tube be now
bent, either upwards or downwards, on looking
into the tube, it will be found perfectly dark; the
light coming in at the bent end will not turn
a corner, and, consequently, none of it reaches
the eye. The annexed engraving of a beam of
light proceeding from a candle will illustrate the
fact of light proceeding in right lines.
LIGHT PRODUCED FROM QUARTZ STONES.
219. If two of these stones (milk stones, as
boys sometimes call them) be struck against each
other, they will emit light; and if they are struck
under water, the same effect will be produced.
TO OBTAIN A LIGHT FROM LOAF SUGAR.
220. If two large pieces of loaf sugar (the
larger the better) be struck against each other in
the dark, a light blue flame, \ike lightning, will
be produced. The same effect takes place when
a grocer chops up a lump of sugar i^th his iron
hatchet, only it is not often noticed.
TRANSPARENCY OP GOLD.
221. All opaque substances might become trans
parent it they could be made sufficiently thin;
and what it is in the constitution of one mass, as
compared with another, which fits the former to
transmit light, and the latter to obstruct it, can-
not clearly be explained ; but we perceive that the
arrangement of the particles has more influence
than their peculiar nature. Nothing is more
opaque than thick masses of the metals ; but
. nothing is more transparent than equally thick
masses of the same metals in solution, nor than
the glasses, of which a metal forms a large pro.
portion. The thousand salts formed by the
union of the metals, or earths, with the diluted
acids, are all transparent when, in cooling from
the fluid to the solid state, their particles have
been allowed to arrange themselves according to
the laws of their mutual attraction—that is to
say, to form crystals; but the same substances in
other states, as when reduced to powder, arc
opaque. Even the metals themselves when re-
duced to leaves of great thinness, arc transparent,
as may be perceived by looking at a lamp through
a fine gold leaf. The light will be visible, but
the flame will appear of a greenish hue.
REFRACTION OF LIGHT.
222. A beam of light passing the atmosphere
into any denser medium, such as water, or glass,
or even into a heavier gas, is bent, or refracted
(see Introduction, 206;) and light passing from a
dense into a lighter medium, suffers an opposite
change in its direction. Refraction, however,
does not take place if the light falls perpendicu-
larly upon a surface ; it is only when it falls ob.
liquely, that it is bent out of its course. The
following experiments will illustrate the refraction
or bending of light by water.
223. Place a coin in a vessel, so that on stand-
ing at a certain distance off, it is just hid by the
edge of the
vessel. Then
get some one
to pour wa-
ter into it,
and the coin
will imme-
diately be-
comevisible;
it will appear to have moved from the side to the
middle of the vessel as shown by the cut.
224. If a basin, or other vessel, be placed so
that a ray of the sun shall fall low on one side
within it, on filling it up with water, the image of
the sun will appear shinning on the bottom of the
vessel; the water having refracted ihe beam of
light which fell on the side so much, that it then
falls on the bottom.
225. Place a stick upright in a tub, and after-
wards fill it up with water; or place a stick in a
vessel of water, and it will appear bent and crooked.
226. A ray of
light which pasaes B
through a piece of
plate glass will suf-
fer considerable re-
fraction, after the
manner represent-
ed in the annexed
engraving, where
a is the piece of
glass, c and d the
parts where the ray enters and emerges, falling on
e ; and the dotted line shows the degree of re-
fraction,
a natural camera obscura.
227. The human eye is a camera obscura ; for
on the back of it, on the retina, every object in a
landscape is beautifully depicted in miniature
Philosophical Experiments.
67
(see Introduction.) This may be proved by pro-
curing a bullock's eye, and carefully removing, or
thinning, the outer coat of it behind, taking care
not to cut it, or the vitreous humor will escape,
and the eye be rendered useless. If the pupil of
it be directed to any bright objects, when it is thus
prepared, they will appear beautifully distinct in
miniature on the back part, precisely the same as
objects appear in the camera obscura. The ef-
fect will be hightened if the eye is viewed in a
dark room, with a small hole in the shutter; but
in every case the appearance will be very strik-
ing.
HOW TO MAKE A CAMERA OBSCURA.
228. This is a very pleasing and instructive lit-
tle piece of apparatus, and may be purchased for
three or four shillings. As some of our readers,
however, may like to make one themselves, and
as this may be done at a very trifling expense,
we give the following directions for the purpose :
Make an oblong box, about a foot long, six inches
wide, and three or four high ; at one end make a
round hole, in which fix a small magnifying glass,
which may be obtained at any optician's. Then,
at the other end, place a piece of looking-glass,
slantingly, so that when the light falls on it after
passing through the magnifying glass, it may be
reflected to the top of the box, near the end. On
this part place a piece of ground glass, or trans-
parent oiled paper, and, after covering the re-
mainder of the top with wood, and blacking the
inside with ink all over, the camera obscura is
complete. On pointing the end of the box to a
landscape, the light will pass through the lens,
and every tiling will appear beautifully distinct,
in miniature, on the ground glass. If, therefore,
a piece of writing paper be placed on it, a very
pleasing drawing may be made with a pencil;
and thus the camera obscura may be made an
endless source of pleasure and instructive amuse-
ment. The wood cut represents a section of the
apparatus; a, is the lens; b, the back, against
which rests the looking-glass; and c is the ground
glass, on which the paper is laid,
DARK SPOT ON THE RETINA--INSENSIBILITY OF THE
OPTIC NERVE.
229. There are few persons aware, that when
they look with one eye, there is some particular
object before them to which they are absolutely
blind. If we look with the right eye, this point
is always about 15° to the right of the object
which we arc viewing, or to the right of the axis
of the eye, or the point of most distinct vision.—
If we look with the left eye, the point is far to the
left. In order to be convinced of this curious
fact, which was discovered by M. Mariotte, place
two colored wafers upon a sheet of white paper,
at the distance of three inches apart, and look at
the left-hand wafer with the right eye, at the dis-
tance of eleven or twelve inches, the experimenter
standing in front of the wafers, taking care to
keep the eyes straight above the wafer, and the
line which joins the eyes parallel to the line which
joins the wafers. When this is done, and the left
eye closed, the right-hand wafer will no longer be
visible. The same effect will be produced if we
close the right eye, and look with the left eye at
the right-hand wafer. When we examine the re-
tina, to discover to what part of it this insensi-
bdity to light belongs, we find that the image of
the invisible wafer has fallen on the base of the
optic nerve, or the place where this nerve enters
the eye, and expands itself to form the retina,
which is a kind of network-expansion of the op-
tic nerve over the interior coat of the eye, and is
the part on which impressions are made, that
render external objects visible to us (see Introduc
tion.)
230. If the above experiment be performed
with candles, instead of wafers, the candle on
either side wdl not entirely disappear, but leaves
behind a faint, cloudy light, without, however,
giving any thing like an image of the object from
which the light proceeds. From a knowledge of
the preceding facts we might, perhaps, be led to
imagine, that on viewing a landscape, whether we
use one or both eyes, to see a black or dark spot
within fifteen degrees of the point which most
particularly attracts our notice. The Divine Ar-
tificer, however, has not left his work thus imper-
fect. Though the base of the optic nerve is in-
sensible to light that falls directly upon it, yet it
has been made susceptible of receiving luminous
impressions from the parts which surround it;
and the consequence of this is, that when the wa-
fer disappears, the spot wliich it occupied, in place
of being black, has always the same color as the
ground upon which the wafer is laid—being
white when the wafer is placed upon a white
ground, and red when it is placed upon a red
ground. This curious effect may be rudely il-
lustrated, by comparing the retina to a sheet of
blotting-paper, and the base of the optic nerve to
a circular portion of it, covered with a piece of
sponge. If a shower falls upon the paper, the
protected part will not be wetted by the rain
which falls upon the sponge that covers it; but
in a few seconds it will be as effectually wetted
by the moisture wliich it absorbs from the wet pa-
per with which it is surrounded. In like man-
ner, the insensible spot on the retina is stimulated
by a borrowed light; and the apparent defect is
so completely removed, that its existence can be
determined only by the experiment already de-
scribed.
CURIOUS EFFECT OF INDIRECT VISION.
231. When the eye is steadily occupied in
viewing any particular object, or when it takes a
fixed direction, while the mind is intently en-
gaged on any subject of contemplation, it sud-
denly loses sight of, or becomes blind to, objects
seen indirectly, or upon which it is not fully di-
rected. In order to witness this illusion, put a
little bit of white paper on a green cloth, and
within three or four inches of it place a narrow
strip of white paper. At the distance of twelve
or eighteen inches, fix one eye steaddy upon the
little bit of white paper, and in a short time a
part, or even the whole of the strip of paper will
63 Philosophical Experiments.
vanish, as if it had been removed from the green
cloth. It will again appear, and again vanish ;
the effect depending greatly upon the steadiness
with which the eye is kept fixed. This illusion
takes place when both the eyes are open, though
it is easier to observe it when one of them is clo-
sed. Tlie same thing happens when the object is
luminous, instead of being a bit of paper. When
a candle is thus seen by indirect vision, it never
wholly disappears, but it spreads itself out into a
cloudy mass ; the centre of which is blue, encir-
cled with a bright ring of yellow light.
ILLUSION OF THE EYE WITH RESPECT TO THE SITU-
ATION OF OBJECTS.
232. Take a ring, of about an inch in diame-
ter, and suspend it from a piece of string, so that
it may hang on a level with the middle of the
face, and with the edge toward the eyes, so that
the orifice of the ring cannot be seen. If one
eye be then closed, it will be found nearly impos-
sible to thrust the end of a stick through the
ring, as the eye will be deceived with regard to
the situation of the ring; although this may be
accomplished easily when both eyes are open.
THE MAGIC LANTERN.
233. This well-known and pleasing philosophi-
cal toy is so great a favorite, that it requires no
recommendation to introduce it to the notice of
the student in optics. Its principle will be best
understood from the annexed engraving, showing
the form of the instru-
ment, and the situa-
tion of the lenses em-
ployed. These lenses
are set in a tube, which
can be lengthened or
shortened at pleasure,
in order to adjust the
image of the object on
the wall, or other sur-
face on which it is
projected. Probably,
by the assistance of
the wood cut, some of
our readers may be en
abled to construct a
magic lantern ; and
the pleasure tobe deri-
I ^ve(* **om **w^ ampiy
f-_-/ff!'recompensc for a little
l,M7 trouble. To use it, it
is advisable to hang
up a table-cloth, or
sheet, on a line at a
little distance from
tlie wall of a room, and for the exhibitor to
stand behind it, as by this means he can increase
or diminish the size of the objects at pleasure, by
adjusting the tube, and standing near, or at a dis-
tance from the cloth. Grotesque figures, ani-
mals, &c, painted on glass slides, having the
other parts covered with black varnish, to pre-
vent the transmission of light, except through
the figure, are generally used to exhibit the pow-
ers of the magic lantern, and may be made with
a little ingenuity, or purchased at the optician's,
where the lenses may also be obtained. Their
situation will be seen from the cut.
DURATION OF IMPRESSIONS ON THE RETINA--THE
CIRCLE OF FIRE.
234. It was formerly thought that these im-
prcssions disappeared from the retina the moment
the object that produced them was removed from
before the eye; but this is found not to be the
case, for an impression—that is to say, a pic-
ture in miniature of any thing held before our
eyes—remains on the retina about the sixth part
of a second after the body that produced it has
been withdrawn (sec Introduction). This may
appear so very inconsiderable a portion of time,
as hardly to be of much importance; but it ena-
bles us to explain the cause of many striking phe-
nomena connected with vision, that would other-
wise be inexplicable. The following pleasing ex-
periments may be performed, to show the effect of
the retina retaining an image of an object after
it is withdrawn from before the eye:—Take a
short piece of wood, and, having burnt one end
of it, so that it shall remain luminous, tic it to a
piece of string, and swing it rapidly round in a
circle. The effect will be, that we shall perceive
a complete circle of fire. If a piece of ignited
charcoal be fixed to the rim of a wheel, to wliich
a rapid motion is then given, the same effect will
be produced, The cause of this appearance will
be understood from the preceding observations.
Tlie eye is fixed on a particular part of the wheel
where the charcoal is placed, and the image of
the burning charcoal will remain on the retina
the sixth part of a second : it is evident, there-
fore, that if we can turn the wheel so rapidly that
the charcoal shall revolve and reach the spot on
which our eye is fixed in less time than this, that
we shall not be informed, by our eyes, of its hav-
ing moved at all; for an image of the burning
charcoal will be constantly on the retina. As it
does not matter on what part of the wheel we
place our eyes to perceive the same effect, the
consequence is, that the whole of the rim of the
wheel appears on fire.
THE THAUMATHROPE.
235. Dr. Paris designed a very pleasing toy to
illustrate the property of the retina", described in
the last experiment; it is called " the thaumath-
rope, and may be easily constructed in a variety
of forms, by the exercise of a little ingenuity.—
The toy may be purchased, but we advise the
reader to make it himself; which may readily be
done from the following directions:—Cut a piece
of card round, about the size of half a crown,
and fix a piece of thread on opposite sides of the
circumference; then paint on one side of the
card some little object, such as a man without a
hat, and on the other side, near the top, a hat by
itself, reversed. Now, on twisting the card
quickly round, by means of the threads, the hat
\vdl appear on the man's head; for the impres-
sion of one side of the card on the retina will not
have ceased before the other side is presented to
Philosophical Experiments.
69
the eye. A variety of objects may be painted on
the card ; such as a mm and a horse (as in the
above cut), a juggler and a number of balls, two
men with drawn swords, &c. Indeed, there arc
a few philosophical toys that afford better oppor-
tunities for the display of taste and ingenuity
than the thaumathrope.
COMPOSITION OF LIGHT.
236. A beam of light, passing through a prism,
is decomposed; and if the rays be received on a
sheet of white paper, they will appear of the
same number and colors as they do in the
rainbow; viz. red, orange, yellow, green, blue,
indigo, and violet. It is supposed by philosophers,
in the present day, that the orange, green, and in-
digo colors are not elementary, like the others, but
arc formed by the mixture of the rays from the
red and yellow, yellow and blue, and blue and
violet parts of the spectrum. Sir Isaac Newton
first proved that white light was not one color, as
had previously been supposed ; and its composi-
tion may be pleasingly illustrated in the follow-
ing manner :—Paste a sheet of white paper on a
circular piece of board, about six inches in diam-
eter, and divide it, with a pencil, into fifty parts
(see cut). Then paint a portion, equal to six
parts, of a red color; four parts, orange; seven,
yellow ; eight, green; eight, blue ; six, indigo ;
and eleven, violet. The colors should be of a
dark tint in the centre, and gradually become
fainter at the edges, till they mix with the one
adjoining. If the board be then fixed on an axle,
and made to revolve quickly, the colors will no
longer appear separate and distinct, but becoming
gradually less visible, they will ultimately appear
white, giving this appearance to the whole sur-
face of tlie paper.
LONG-CONTINUED IMAGE OF THE SUN ON THE RE-
TINA.
237. The experiments just mentioned will be
sufficient to illustrate a few of ,the curious effects
that are produced, in consequence of objects re-
maining on the retina after they have been re-
moved from before the eye; but, occasionally, ef-
fects of a very alarming character have been pro-
duced from the same cause ; and as it is certain
that nearly all ghosts and apparitions, which per-
sons have asserted they have seen, existed in their
eyes, in consequence of circumstances connected
with this particular property of the eye, the fol-
lowing account of an experiment, performed by
Sir Isaac Newton, may be both entertaining and
useful. Any of our readers may perform a simi-
lar experiment by looking, for some time, steadily,
at a burning body, such as a candle, for exam-
ple ; but, prob ibly, after reading the following an-
ecdote, they will be content without personally
performing the experiment.
238. Mr. Boyle having mentioned, in his
" Book on Colors," an individual who continued,
for years, to see the sun whenever he looked upon
bright objects, in consequence of having once
steadily contemplated that luminary for a consid-
erable period, Locke mentioned the case to New-
ton, who gave the following account of a similar
occurrence that had happened to himself:—" The
observation you mention in Mr. Boyle's ' Book
of Colors,' I once made upon myself, with the
hazard of my eyes. The manner was this: I
looked, a very little while, upon the sun in the
looking-glass, with my right eye, and then turn-
ed my eyes into a dark corner of my chamber,
and winked to observe the impression made, and
the circles of colors wliich encompassed it, and
how they decayed by degrees, and at last vanish-
ed. This I repeated a second and a third time.
At the third time, when the phantasm of light,
and colors about it, were almost vanished, intend-
ing my ftincy upon them to see their last appear-
ance, I found, to my amazement, that they began
to return ; and, by little and little, to become as
lively and vivid as when I had newly looked upon
the sun. But when I ceased to intend my fancy
upon them, they again vanished. After this, I
found that as often as I went into the dark, and
intended my mind upon them, as when a man
looks earnestly to see any thing that is difficult to
be seen, I could make the phantasm return, with-
out looking any more upon the sun; and the oft-
ener I made it return, the more easily I could
make it return again : and at length, by repeat-
ing this, without looking any more upon the sun,
I made such an impression on my eye, that if I
looked upon the clouds, or a book, or any bright
object, I saw upon it a round, bright spot of fight,
like the sun ; and, which is still stranger, though
I looked upon the sun with my right eye only, and
not my left, yet my fancy began to make an impres-
sion on my left eye, as well as upon my right: for
if I shut my right eye, and looked upon the clouds,
or a book, with my left eye, I could see the spec-
trum of the sun almost as plain as with my right
eye, if I did but intend my fancy a little time
upon it; for at first, if I shut my jight eye, and
looked «vith my left, the spectrum of the sun did
not appear till I intended my fancy upon it; and,
by repeating this, appeared every time more ea-
sily. And now, in a few hours time, I had
brought my eyes to such a pass, that I could
look upon no bright object with either eye, but I
saw the sun before me, so that I durst neither
write nor read; but to recover the use of my
eyes, shut myself up in my chamber, made dark,
for three days together, and used all means in my
power to direct my imagination from the sun;
for if I thought upon him, I presently saw his
picture, though I was in the dark. But, by
keeping in the dark, and employing my mind
about other things, I began, in three or four days,
to have more use of my eyes again; and by for-
bearing to look upon bright objects, recovered
them pretty well—but not so well but that, for
some months after, the spectrums of the 6un be-
gan to return as often as I began to meditate
*0
Philosophical
Experiments.
upon the phenomenon, even though I lay in bed
at midnight, with my curtains drawn. But now
I have been well for many years; though I am
apt to think, if I durst venture my eyes, I could
still make the phantasm return, by the power of
my fancy." This experiment proved how easily
the image of a bright object might be recalled,
and the mind be deceived by an appearance that
was not real. There can be no doubt but that
persons have often, in this manner, had the forms
of deceased friends recalled so vividly, that they
have appeared to be actually present; and per-
sons not acquainted with the fact that the eye
can deceive the mind in this way, would never
doubt the reality of what they thought they saw.
TO READ THE INSCRIPTION OF A COIN IN THE DARK.
239. To do this, take a silver coin, and after
polishing the surface as much as possible, make
the parts of it wliich are raised rough, by placing
on them a little oil of vitriol, or some other acid;
the parts not raised are to be left polished. If the
coin thus prepared is placed upon a mass of red-
hot iron, and removed into a dark room, the in-
scription upon it will become distinctly visible,
and may be read by a spectator. The mass of
red-hot iron should be concealed from the observ-
er's eye, by having something placed before it,
both for the purpose of rendering the eye fitter
for observing the effect, and of removing all doubt
that the inscription is really read in the dark ;
that is, without receiving any light, direct or re-
flected, from any other body. If, instead of rough-
ening the raised parts of the coin by an acid, we
polish the raised parts and roughen the depressed
parts, we shall still be able to read it, from its be-
ing, as it were, written in black letters upon a
white ground—the reverse of the first experiment.
TO READ THE INSCRIPTION THAT HAS BEEN ERASED
FROM A COIN.
240. When such a coin is laid upon the red-
hot iron, the letters and figures that have been
either wholly obliterated, or obliterated to such a
degree as to be illegible, become oxidated, or rust-
ed ; and the film of oxide radiating more power-
fully than the rest of the coin, the illegible in-
scription may be now distinctly read, to the great
surprise of an observer who had previously ex-
amined the blank surface of the coin.
241. In order to explain the cause #f this re-
markable phenomenon, and that of the previous
experiment, it is necessary to notice a method,
that has been long known, of deciphering the in-
scriptions on worn-out coins. This is done by
merely placing the coin upon a hot iron; an oxi-
dation takes place over the whole surface of the
coin, the film of oxide changing its tint with the
intensity or continuance of the heat. The parts,
however, where the letters of the inscription had
existed, oxidate at a different rate from the sur-
rounding parts; so that these letters exhibit their
shape, and become legible, in consequence of the
film of oxide which covers them having a differ-
ent thickness, and therefore reflecting a different
tint from that of the surrounding parts. The
tints thus developed sometimes pass through ma-
ny orders of brilliant colors—particularly pink
and green, and settle in a bronze, and sometimes
a black tint, resting upon the inscription alone.
When the experiment is often repeated, the coin
loses its property of becoming luminous in this
way; but regains it on being exposed for a lime
to the atmosphere. The reason that the parts of
a coin, that hus been roughed by an acid, become
more luminous than the parts that are left in a
polished state, is, because all black and rough sur-
faces radiate light more copiously than polished
and smooth surfaces ; and hence the inscription
is luminous when it is rough, and obscure when
it is polished.
LAUGHABLE EFFECT OF HOMOGENEOUS LIGHT.
242. An experiment, productive of much
amusement, and at the same time well illustrat-
ing the cause of colors, may be performed with
homogeneous light. If a little spirits of win«—
or some spirit, such as gin—be ignited in a dish,
and a quantity of common table salt thrown on
it, the lights in the room having been previously
put out, every person present will have a most
ghastly look, and their clothes will assume an ex-
traordinary color; the hue of health will disap.
pear from the cheeks, and the different articles of
clothing will entirely change their complexion.—
The cause of this phenomenon will be found in
the circumstance, that the color of bodies depends
upon the rays of light being partly absorbed, and
partly reflected. A ray of white light can be
shown to consist of seven prismatic colors, as
they are called (see experiment 246), and differ-
ent bodies possess the power of absorbing one or
more of these colors, and reflecting all the rest;
and the combination of the rays that are reflect-
ed gives the particular color to an object. Red-
colored bodies, for instance, absorb all the rays,
except the red ray ; and tliis accordingly appears
to be the color of the body—and so on of all other
colors. When, therefore, homogeneous light is
produced by the means above mentioned, as the
articles of dress, and the faces of the company,
do not absorb all the yellow rays, but reflect a
portion, the color of every thing is changed.
243. If we were to illuminate scarlet cloth
with pure and unmixed yellow light, it would ap-
pear yellow, because the scarlet cloth does not
absorb all the yellow rays, but reflect some of
them ; and if we illuminate blue cloth with yel-
low light, it will appear nearly black, because it
absorbs all the yellow light, and reflects hardly
any of it. But, whatever be the nature and co-
lor of the bodies on which the yellow light falls,
they must appear yellow ; for no other light falls
upon them, and those which are not capable of
reflecting yellow fight must appear absolutely black,
however brilliant be their color in the light of day.
This is the cause of the curious appearance of
the company when homogeneous light is pro-
duced, as above mentioned.
HEAT OF THE COLORS OF THE SPECTRUM.
244. The heating powers of the rays of the
solar spectrum arc found to be of different de-
grees. If the bulb of an air thermometer be
moved in succession through the differently-col-
ored rays, it wdl be found to indicate the greatest
heat in the red rays; next in the green ; and so
on, in a diminishing progression, to the violet.
TO SHOW THAT LIGHT AND HEAT ARE DISTLNCT IN
THE SIN'S RAYS.
245. If the thermpmeter be removed entirely
Philosophical Experiments.
71
out of the confines of the red rays, but with the
bulb still in the line of the spectrum, it rises even
higher than in the red rays, and continues to rise
till removed half an inch beyond the extremity
of the red ray. In this situation, quite out of the
visible light, the thermometer has been known to
rise, in two minutes and a half, from 61 degrees
to 70 degrees. The ball of the thermometer em-
ployed should be extremely small, and be black.
cned over with India Ink.
PRISMATIC COLORS.
246. Cut a small slit
in a window-shutter (a,)
on wliich the sun shines
at some period of the
day; and directly op.
posite the hole, place a
prism (p). A beam of
light,in passing through
it, will be decomposed;
and if the light fall on
a sheet of paper, or
against a white wall,
the seven colors of the
rainbow will be ob-
served, as in the en-
graving (see Introduc-
tion.)
247. If the split in
the window-shutter be
very small, and no
prism is placed oppo-
site to it, only four col-
ors will appear—viz.
red, green, yellow, and violet.
OCULAR SPECTRA, OR ACCIDENTAL COLORS.
248. If we cut a figure out of red paper, and,
placing it on a sheet of white paper, view it stea-
dily for some seconds, with one or both eyes fixed
on a particular part of it, we shall observe the
red color to become less brilliant. If we then
turn the eye from the red figure upon the white
paper, we shall see a distinct green figure, which
is the spectrum, or accidental color of the red fig-
ure. With differently-colored figures, we shall
observe differently-colored spectra, as in the fol-
lowing table:—
Color of the originalfigurc: Color of the spectral figure.
Red..................Blueish Green.
Orange................Blue.
Yellow..................Indigo.
Green................... Reddish Violet.
Blue.................Orange Red.
Indigo............... Orange Yellow.
Violet......• • •......Yellow.
Whit.-...............Black.
Black................White.
249. The two last of these experiments, viz.,
white and black figures, may be satisfactorily
made by using a white medallion on a dark ground,
and a black profile figure. The spectrum of the
former will be found to be black, and that of the
latter white.
250. These ocular spectra often show them-
selves without any effort on our part, and even
without our knowledge. In a highly-painted
room, illuminated by the sun, those parts of the
furniture on which the sun does not directly fall,
have always the opposite, or accidental color. If
the sun shines through the chintz in a red win-
dow-curtain, its light will appear green, varying,
as in the foregoing table, with the color of the
curtain ; and if we look at the image of a can-
dle, reflected from the water in a blue finger glass,
it will appear yellow. Whenever, in short, the
eye is affected with one prevailing color, it sees,
at the same time, the spectral or accidental color,
just as when a musical string is vibrating, the
ear hears, at the same time, its fundamental and
its harmonic sounds.
PHOSPHORESCENCE OF THE SEA ILLUSTRATED.
251. The sea frequently presents a very beau-
tiful phosphorescent appearance, which arises, in
most cases, from the presence of innumerable
quantities of exceedingly minute living creatures,
like glow-worms, furnished with the means of be-
coming phosphorescent. The effect they pro-
duce may be imitated with a basin of water, in
the following manner:—Pour a little phospho-
retted ether on a lump of sugar, and drop it into
the water, which should be made lukewarm. In
a dark place, the surface of the water will soon
become luminous; and if it be moved, by blow-
ing gently with the mouth, beautiful and brilliant
undulations of the surface will be visible, exhib-
iting the appearance of liquid combustion. Those
who cannot see the ocean in a flame, may adopt
this method of feebly imitating it; and it will
serve to give them a faint idea of a phenomenon,
which has called forth the admiration of all who
have ever seen it.
PHOSPHORESCENCE OF THE RETINA.
252. A class of ocular deceptions have their
origin in a property of the eye, and they have
been very imperfectly examined. The fine ner-
vous fabric which constitutes the retina, and
which extends to tlie brain, has the singular prop-
erty of being phosphorescent by pressure. When
we press the eye-ball outward, by applying the
point of the finger between it and the nose, a cir-
cle of light will be seen, which Sir Isaac Newton
describes as " a circle of colors, like those in the
feather of a peacock's tail." He adds, that " if
the eye and the finger remain quiet, these colors
vanish in a second of time; but if the finger be
moved, with a quavering motion, they appear
again." The luminous circles always continue
while the pressure is applied, and they may be pro-
duced as readily after the eye has been long in
darkness, as when it has been recently exposed to
light. When the pressure is very gently applied,
so as to compress the fine pulpy substance of the
retina, light is immediately created, when the
eye is' in total darkness; and when in this state,
light is allowed to fall upon it: the part com-
pressed is more sensible to light than any other
part, and, consequently, appears more luminous.
If we increase the pressure, the eye-ball, bemg
filled with incomprehensible fluids, will protrude
all round the point of pressure; and, consequent-
ly, the retina, at the protracted part, will be com-
pressed by the outwurd pressure of the contained
fluid, while the retina on each side—namely, un-
der the point of pressure, and beyond the protru-
ded part—will be drawn toward the protruded
part, or dilated. Hence, the part under the fin-
ger, which was originally compressed, is now di-
lated; tie adjacent parts compressed, and the
72
Philosophical Experiments.
more remote parts immediately without this, di-
lated also.
253. Now we have observed, thrrt when the eye
is, under these circumstances, exposed to light,
there is a bright, luminous circle shading off, ex-
ternalby and internally, into total darkness. We
are led, therefore, to the important conclusions,
that when the retina is compressed in total dark-
ness, it gives out light; that when it is com-
pressed while exposed to light, its sensibility to
light is increased ; and that when it is dilated,
under exposure to light, it becomes absolutely
blind, or insensible, to all luminous impressions!
254. When the body is in a state of perfect
health, this phosphorescence of the eye shows it-
self on many occasions. When the eye-ball, or
the eye, receives a sudden blow, a bright flash of
light shoots from the eye-ball. In the act of
sneezing, gleams of light are emitted from each
eye, both during the inhalation of the a>r, and
during its subsequent expulsion ; and in blowing
air violently through the nostrils, two patches of
light appear abeve the axis of the eye, and in
front of it, while other two luminous spots unite
into one, and appear, as it were, about the point
of the nose when the eyes are directed to it.—
When we turn the eye-ball, by the action of its
own muscles, the retina is affected at the place
where the muscles are inserted ; and there
may be seen, opposite each eye, and toward the
nose, two semicircles of light, and other two, ex-
tremely faint, toward the temples. At particular
times, when the retina is more phosphorescent
than at others, these semicircles are expanded
into complete circles of fight. In a state of in-
disposition, the phosphorescence of the retina ap-
pears in a new and alarming form (see Introduc-
tion). When we consider the variety of distinct
forms which, in a state of perfect health, the im-
agination can conjure up when looking into a
burning fire, it is easy to conceive how the mass-
es of colored light, which often float before the
eyes in illness, may be moulded, by the same pow-
er, into those fantastic shapes that often haunt
the sick man's couch. Sir D. Brewster has ably
illustrated these phenomena in his " Natural
Magic."
SOLAR PHOSPHORI.
255. There are many substances in nature,
which, when heated to a.certain degree, acquire
the property of becoming luminous at low de-
grees of temperature, and when merely exposed
for a time to the sun. Canton's phosphorus,
which is obtained from calcined oyster-shells,
possesses this property; and common oyster-
shells maybe rendered phosphorescent, by attend-
ing strictly to the following directions, which are
given by the discoverer for the purpose:—Take
the most flaming coals off a brisk fire, and throw
in some thick oyster-shells; then replace the coals
and calcine the shells for an hour. Remove them
carefully, and, when cold, it will be found that,
after exposing them for a few minutes to the sun,
they will glow, when taken into a dark room,
with most of the prismatic colors.
256. Fluor spar, several varieties of phosphate
of lime, and marble, become luminous, when
heated to a certain point, without undergoing
combustion. Their luminous property may be
best exhibited, by scattering them, in coarse pow.
der, upon an iron plate, heated to redness.
287. Many animal substances are nuturall)
phosphorescent. This property in the glow-worm
is well known; and it appears that salt-water
fish become luminous in about twelve hours after
death, the brilliancy increasing till putrefaction is
evident, when it decreases. This effect, how-
ever, docs not take place in fresh water.
BREATHING LIGHT AND DARKNESS.
258. The following experiment, if performed
with care, is exceedingly striking, and beauti-
fully exhibits one of the many optical delusions
to which we are liable. Let s be a candle,
whose light falls at an
upon two glass plates,
(a b), placed close tov
each other, and let the re-
flected rays (a c b d) fall
at the same angle upon
two similar plates (c n),
but so placed, that the
plane of reflection from the.
latter is at right angles to
the plane of reflection from
the former. An eye placed
at e, and looking, at the
same time, into the two
plates, c and d, will see
very faint images of the
candle (s), which, by a
slight adjustment of the
plates, may be made to
disappear almost wholly,
allowing the plate c to re-
main as it is; change the
position of d, till its incli-
nation :«the ray b d,
d is diminished about 3^°,
or made nearly 53° 11'.—
This distance may easily
be found by a "little prac-
tice. When this is done,
the image that had disap-
peared on looking into d
will be restored; so that-
the spectator at e, upon looking into the two mir-
rors, c d, will see no light in c, because the can-
dle has nearly disappeared; while the candle is
distinctly seen in d. If, while the spectator is
looking into two mirrors, either he, or another
person, breathes upon them gently, and quickly,
the breath will revive the extinguished image in
c, and will extinguish the visible image in d.—
The following is the cause of this singular re-
suit:—The light a c b d is polarized by reflection
from the plates a b, because it is incident at the
polarizing angle, 56° 45', for glass. When we
breathe upon the plates c d, we form upon their
surface a thin film of water, whose polarizing an-
gle is 53° 11'; so that if the polarized rays, a c
b d, fell upon the plates c d, at an angle of 53°
11', the candle from which they proceeded would
not be visible, or they would not suffer reflection
from the plates c d. At all other angles, the
light would be reflected, and the candle visible.
Now the plate d is placed at an angle of 53° 11',
and c at an angle of 56° 45', so that when a film
of water is breathed upon them, the light will be
Philosophical Experiments. 73
reflected from the latter, and none from the for-
mer; that is, the act of breathing upon the glass
plates will restore the invisible, and extinguish
the visablc image. This is an experiment of
Brewster's.
CHANGES OF THE KALEIDOSCOPE.
259. The following curious calculation has
been made of the number of changes this won-
derful instrument wdl admit:—Supposing the in-
strument to contain 20 small pieces of glass, &.c,
and that you make 10 changes in each minute, it
will then take the inconceivable space of 462,-
880,899,576 years, and 360 days, to go through
the immense variety of changes it is capable of
producing; amounting (according to our frail
idea of the nature of things) to an eternity. Or,
if we take only 12 small pieces of glass, and
make 10 changes in each minute, it will then
take 33,264 days, or 91 years and 49 days, to ex-
haust its variations.
HEAT OR CALORIC.
Introduction to the science of heat—Theories of heat—Gen-
eral effects of heat in nature—Heat the antagonist to at-
traction—Latent heat—Sources of heat—Combustion—
Haat of the sun—Heat produced by friction—Heat by per-
cussion—Heatby chemical mixture—Heathy electricity and
Galvanism—Heatby animals—Spontaneous combustion—
Properties of heat—Expansion of bodies—Heat—Tendency
of Hea to equilibrium—Summary of the properties of heat.
260. Heat, or caloric, as it is philosophically
termed, is the most active principle in nature ;
there is not a chemical change that takes place,
in which it is not concerned, and, without it, vi-
tality would become extinct. Wc are all famil-
iar with the sensation it causes, and philosophers
have been able to determine with exactness, the
various phenomena it is capable of producing;
but this is all that has been done, for we are as
ignorant, in the present day, of what heat really
is, as the first phUosopher who turned his atten-
tion to the subject. The reason of this is, that
heat has never been exhibited by itself, apart from
material bodies ; it is always found in combina-
tion with them, and we can, therefore, only judge
of its effects. Many theories have, however,
been proposed, from time to time, to explain the
principle of heat; but, for the reason above sta-
ted, they have been necessarily unsupported by
facts, and were merely suggestions of the au-
thors.
By some, heat has been thought to be particles
of matter that are shut off from burning bodies
with amazing velocity; but wliich, being infi-
nitely small, are incapable of injuring our most
delicate organs. Others, again, suppose that it is
no material substance, but only the effect pro-
duced by certain vibrations among the particles
of which all bodies are composed. Both these
theories are, however, incapable of proof; and as
all the phenomena of heat can be perfectly un-
derstood, without any thing of itself as a princi-
ple, the student need pay little regard to either of
the theories just mentioned, or puzzle himself in
endeavoring to understand its essence.
261. Dr. Arnott beautifully describes the gen-
eral effects of heat in his treatise on that sub-
ject. " In the winter of climates," says he,
" where the temperature is, for a time, below the
freezing point of water, the earth, with its wa-
ters, is bound up in snow and ice ; the trees and
shrubs are leafless, appearing every where like
withered skeletons; countless multitudes of liv-
ing creatures, owing either to the bitter cold, or
deficiency of food, are perishing in the snows—
nature seems dying, or dead: but what a change
when spring or heat returns ! The earth is again
uncovered and soft; the rivers flow ; the lakes are
again liquid mirrors ; the warm showers come to
foster vegetation, which soon covers the ground
with beauty and plenty. Man, lately inactive,
is recalled to many duties: his water-wheels are
every where at work; his boats are again on the
canals and streams ; his busy fleets of industry
are along the shores. Winged life, in new mul-
titudes, fills the sky; finny fife similarly fills the
waters; and every spot of earth teems with vi-
tality and joy. Many persons regard these
changes of season as if they came like the suc-
cessive positions of a turning-wheel, of which
one necessarily brings the next; not adverting
that it is the single circumstance of change of
temperature which docs all. But if the cold of
winter arrive too early, they unfailingly produce
the wintry scene; and if warmth come before its
time in spring, it expands the bud and the blos-
som, which a return of frost will surely destroy.
A seed sown in an ice-house never awakens to
life."
262. Heat is the great antagonistic force in
nature opposed to attraction. While the effect
of the latter is to draw the particles of matter in
closer contact with each other, the effect of heat
is to make them separate; and hence, on the
power of heat depends the different states in
which bodies are found, either as solids, liquids,
or gases. It is well known that, if we apply heat
to a lump of ice, it melts and becomes water;
and if we continue the heat, this water becomes
a gas, called steam. In this instance, therefore,
heat is capable of producing all the different
states in which matter is found existing in na-
ture ; and the experiment proves that it is heat
which causes matter to assume these forms.—
Water, in its natural state, is liquid; yet the ab.
straction of the heat peculiar to it, as water, at
once reduces it to the solid form; and, in some
parts of the world, this is the only state in which
it is found. Within the tropics, on the contrary,
ice, and its different modifications, snow, hail,
&c, are never seen ; so that a person, wishing to
send a friend within this latitude the greatest cu-
riosity he could from England, packed up a box
of snow ! He was unable, however, to make the
box as impervious to heat as an ice-house; and
the only curiosity the friend found, therefore, on
opening the box, was a cupful of water! When
natives of India, and similar hot countries, ar-
rive in England, nothing occasions them greater
surprise than to see water in a solid state; and it
is said that an eastern monarch, having called a
traveller before him to relate what he had seen in
foreign countries, forgave him all the falsehoods
he thought he had uttered, until the traveler told
him that, in some places, water becomes natu-
rally hard, and could be cut like blocks of mar-
ble for several months of the year; upon which,
the monarch ordered him instantly to be put to
death, for endeavoring to deceive him by the re-
.*<*
46 Philosophical Experiments.
lation of what it was impossible could ever hap-
pen.
263. The sensation we experience on approach-
ing a burning body, at once informs us of the ex-
istence of heat; but it exists also in all bodies,
in a state in which it is insensible to the touch,
and in which condition it has no effect upon the
thermometer. In this state, it is called latent
heat. In the following pages, numerous instan-
ces are given of its existence in this form, which
will enable the reader easily to understand the dif-
ference between this and sensible heat; but, in
order to explain it briefly here, we may allude
again to the changes that take place in water, as
illustrations. If an uncovered vessel, containing
water, be placed upon the fire, the heat will soon
make it boil; and if a thermometer be then pla-
ced in it, it will indicate 212 degrees. Now,
if the heat be ever so much increased, while the
vessel remains uncovered, the water wdl never
become hotter than this ; but it will soon evapo-
rate in the form of stearn, and all the additional
heat applied, after the water has reached a tem-
perature of 212 degrees, is-.absorbed, to form
steam; or, in other words, becomes the latent
heat of steam. We might suppose that the steam
would be hotter than the water, as it receives all
this additional heat; but if the thermometer be
held in the steam it will not rise higher than 212
degrees: this is because all the heat absorbed by
. the steam has become hMent; and if we cool
A steam, so that it shall retuR to its original state,
as water, it will give out* the exact quantity of
heat that it required in order to assume the form
of steam. The more solid a' body becomes, the
more latent heat it gives out; so water, when it
changes to ice, allows its latent heat to escape:
and before ice can again become water, it must
absorb a sirmlar quantity to that previously evol-
ved. The temperature of ice is 32 degrees, and
water will not freeze until it is cooled to that
point; it will not freeze at 33 degrees. We
might, therefore, suppose that, by adding one de-
gree of heat to ice, we could change it into wa-
ter ; but, in fact, it requires one hundred and for-
ty degrees, as one hundred and thirty-nine de-
grees become latent, and we cannot ascertain its
presence by the thermometer, or by the touch.
Latent heat exists in all bodies, however cold
they may feel; and whenever they are compress-
ed, a portion of this heat will be squeezed out, in
the same way that we may squeeze out water
from a sponge, although, to the sight, it may ap.
pear nearly dry. It will be found, therefore, in
the following experiments, that whenever a body
is subjected to pressure, heat is forced out; and
this will be found the case, not merely with solid
bodies, but with liquids, and even with the air it-
self. (See experiment 284.) The principal sour-
ces of heat are, combustion, the sun, friction,
percussion, chemical mixture, and Galvanism.—
Animals, also, have the power of generating heat
during respiration; and there are other means by
which it is occasionally produced, such as com-
pression, and what is termed spontaneous com-
bustion ; by which animal bodies are consumed
without any apparent cause.
264. Combustion is the artificial means more
generally adopted to produce heat. Certain bo.
dies in nature—such as wood and coals—are call-
ed combustibles, and when ignited in any gas
which supports combustion—such as the atmos.
phere or oxygen—chemically combine with this
supporter of combustion, and give out much heat
that had previously been latent. Sometimes the
combustion is instantaneous; sometimes it is
slow : this depends on the affinity of the burning
body for oxygen; and in the following experi.
ments, many instances are given of the intense
chemical action that sometimes takes place.—
The laws which regulate combustion are also
fully explained, so that it is unnecessary to refer
to them here. (See experiment 311.)
265. The sun is the principal source of heat,
and it is calculated that heat comes to us from
that luminary at the amazing velocity of 200,000
miles in a second of time—a speed which it i9
impossible for us rightly to comprehend. The
heat of the sun docs not depend on the distance
it is from us ; for, although we are many millions
of miles nearer to it in winter than we are in
summer, yet winter is coldest; because the rays
from the sun fall more obliquely on this part of
the globe, at that season of the year, than they
do in summer. When the rays fall directly on
the earth, there is great heat evolved; and tins is
principally the reason why the climate is always
so hot at the Equator. The heat derived from
the sun differs, in many respects, from that pro.
cured by other means. It passes readfiy through
glass, while the heat from a fire does not. Some
writers have even stated, that artificial heat will
not pass through glass at all; but this is a mis-
take, which any one may ascertain by holding
his hand near a gas-glass, while the gas is burn-
ing : the heat, however, does not pass through
readily, and advantage has been taken of this
circumstance in the manufacture of elegant fire-
screens, by which persons may enjoy " the Eng-
lishman's comfort" of looking at the fire, without
experiencing any unpleasant degree of heat. The
sun's rays have been found, by experiment, to be
divisible into two portions, the one conveying
light, the other heat: and it has been ascertained
these rays are distinct from each other (sec 245);
hence it happens, that the light of the sun may
be reflected from a body, while its heat is absorb-
ed. This is really the case with the moon. The
rays of light proceeding from that luminary are
cold, and not the slightest degree of heat can be
derived from them, even when a number are
made to fall on one spot, by means of a " burn-
ing-glass." A very different effect is produced
when the sun's rays are condensed in a similar
manner: the most intense heat may be produced
by this means; and, by arranging a number of
plain mirrors (looking-glasses) in such a way that
the image of the sun from all of them shall fall
on one spot, a sufficient degree of heat may be
produced, even to melt the metals, gold and pla-
tinum. It was by such an arrangement of mir-
rors, that Archimedes was enabled to set on fire
the shipping of the enemy who besieged Syra-
cuse.
266. Friction is another means of procuring
heat. When two substances are rubbed together,
they become warmer; and in machinery, great
care is obliged to be taken, in order to prevent
any part catching fire from this cause. If a
piece of glass, which is incombustible, be held
Philosophical Experiments. ' 5
against the edge of a grit-stone, while revolving,
the glass will become too hot to hold : this is in
consequence of the friction between the glass
and the stone forcing out a portion of their latent
heat; for it is only in this way we can account
for the heat that is produced. In the experiments
which follow, many instances are given, which
will more fully explain this phenomena. (See ex-
periment 283.)
267. Percussion is the method adopted by
house-wives, with a tinder-box, to procure light;
and its effects are, therefore, pretty well known.
When two bodies are struck together, heat is
given out; and if, as is the case of a flint and
steel, one of the substances happens to be harder
than the other, a portion of the softer substance
will often be melted. In the instance alluded to,
the flint, being harder than the steel, melts a por-
tion of it, which, while red-hot, falls upon the tin-
der, and ignites it; thereby producing sufficient
heat to melt and light the sulphur on the end of a
match. The cause of the heat is supposed to be
the sudden compression which the bodies under-
go, and which forces out a portion of the heat
that had previously been latent. One striking
instance of the effect of percussion is given in
experiment 285. '
268. Chemical mixture is a constant source of
heat, since all experiments in chemistry, in which
the bulk of a body is reduced, produce it; and in
other cases, when the affinity of two bodies for
each other is suddenly developed by chemical
mixture, intense and instantaneous heat is pro-
duced. In some cases, however, intense cold is
produced by mixture : this is in consequence of
the bodies expanding, when, of course, an effect
precisely opposite is produced to that which takes
place when a body is condensed. Chemical ex- j
periments, explaining these facts, are generally |
very striking and beautiful; and numerous ex-
amples will be found in the following pages: it
is necessary, however, to caution the student to !
attend particularly to the directions that are giv- ,
en, and to experiment with very small quantities
of the chemicals to be used, by which means, j
very often, the process will be far more satisfac-
tory, and illustrate the fact much better, than if,
a large quantity were employed.
269. Galvanism and Electricity are the last
means that have been alluded to, when describ-
ing the principal sources of heat; and for pro-
curing an intense degree of artificial heat, Gal-
vanism is the best method that can be adopted.
By its means, all the metals may be fused with
the greatest facility; thereby showing, that the
temperature produced must be aqual to that which
can be derived from the sun. Sir Humphrey
Davy had a Galvanic battery erected for him at
the Royal Institution, by wliich ho was enabled
to fuse every substance exposed to its influence,
and by which he decomposed the various earths,
that had formerly been considered to be simple
bodies, and determined many other important
chemical facts.
270. The temperature of animal bodies is in-
dependent of the surrounding atmosphere, or
other medium in which they live; for it is found
that the heat of the human body is nearly the
same all over the world. Living bodies exhibit a
remarkable difference from unorganized matter in
this respect: the latter soon acquire a tempera-
ture similar to that of the bodies by which they
are surrounded ; for instance, a candle, if brought
into a room, of which the temperature is verv
high, begins to melt; if some water is exposed to
the air, when it is below 30 degrees, the water
is frozen: thus, in both instances, we see how
readily unorganized matter acquires the same
temperature as that of the medium in which it is
placed. This, however, is not the case with liv-
ing bodies ; they maintain an equal temperature,
with very slight variation in summer and winter,
at the Poles, and at the Equator. To do this it
is necessary that they should be enabled, in a
cold climate, to generate a great quantity of heat,
and in a hot climate, to dispose of it readily.—
At present, we have merely to describe the man-
ner in which animals generate heat; but in the
experiments which follow, will be found several
illustrations of the mode in which the supera-
bundant heat is disposed of.. (See 289.)
271. The phenomenon of respiration is analo-
gous, in many respects, to combustion. The
blood circulating in the veins contain a conside-
rable quantity of carbon; and before the blood
can circulate through the body, to perforin its va-
rious functions, it is necessary that this carbon
should be removed. This is effected in the lungs.
The blood is conveyed there, in an impure state,
in very small blood vessels, which are permeable
to the air, and are placed over small globules of
thin cellular tissue, being the terminations of the
windpipe. When we inspire the air, it is con-
veyed to these globules, or air-cells; and, pass-
ing through them, enters the blood: the oxygen
of the air then combines with the carbon, and
forms carbonic acid, just the same as it is form-
ed when we burn a candle, in a glass, under wa-
ter. (See experiment 306). This carbonic acid,
mixed with the nitrogen of the air, is given out
when we expire our breath ; and its qualities may
be proved by experiment 117. Now we know, in
the case of the candle, that the union of its car-
bon with oxygen occasions heat; and the same
effect is produced in the lungs. The formation
of carbonic acid there is attended with the evo-
lution of heat, and this is conveyed by the blood
to every part of the body. (See experiment 309.(
The means by which the same temperature is
maintained by the body, in cold weather as in
hot, are vital; for when we are exposed to cold,
an impulse is given to the function of respiration,
by means of which, the blood is more frequently
brought into contust with the air, and, conse-
quently, a greater degree of heat is generated.
272. Spontaneous combustion can hardly be
enumerated among the general sources of heat,
since it occurs so seldom. Instances are record-
ed, however, in the scientific journals, of several
well-authenticated instances, in which persons
have been discovered burning slowly away, some-
what in the way that phosphorus burns, at a low
temperature, in the atmosphere. It appears, in-
deed, as if the body underwent some change, by
which a considerable portion of it was changed
to phosphorus, or some substance very nearly re-
sembling it. Phosphorus is principally formed
from animal mutter; and the supposition has,
therefore, some support. But, as the instances
when this peculiar mode of generating heat have
*\
76 Philosophical Experiments.
occurred but seldom, philosophers have not had
sufficient opportunities of investigating the phe-
nomenon satisfactorily.
Having thus explained the distinction between
latent and sensible heat, and described the prin-
cipal means by which it is obtained, it only re-
mains for us now to describe generally its effects.
This may be done briefly, because, in the follow-
ing experiments, these are fully illustrated.
273. Heat expands bodies. This is a univer-
sal law, and there are but one or two apparent ex-
ceptions. Were there no such thing as heat, li-
quids and gases could not exist; all matter would
be solid. Heat is the cause of bodies becoming
fluid ; it insinuates itself between the particles of
which they are composed, and forces them fur-
ther apart: if a great degree of heat is applied,
the particles are separated so far, that they then
assume the form of gas. Steam is a familiar ex-
ample ; and the thermometer acts solely on this
principle. There are only two or three excep-
tions to this law, and they are only so in appear-
ance. The principal one is water, which, instead
of contracting when cooled down below 32 de-
grees, expands, when it assumes the form of ice.
This is a beautiful provision, since the ice, float-
ing on the water, prevents it parting readily with
its heat, and thus does not allow our rivers, &c,
to become a solid mass of ice, as they otherwise
would. The cause of the water expanding, and
becoming lighter when it freezes, is because the
crystals of ice have interstices between them,
which are filled with air.
274. Heat has a tendency to equilibrium; it
endeavors to produce, in all bodies, the same de-
gree of temperature: it is, therefore, constantly
given off from objects which are hotter than
those by which they are surrounded—1st, by ra-
diation (see experiment 298): 2dly, by conduc-
tion (see experiments 290,292, 294); 3dly, by re.
flection (see experiment 297). The wonderful
effects produced by these means are fully de-
scribed in the following experiments; and it is
unnecessary, therefore, to do more than allude to
them in this introduction.
EXPERIMENTS IN HEAT.
Sensations of heat—Various theories respecting—Latent heat
—In Iron—In water—In a common button—Developed by
friction—In the air—Production of heat by percussion—
Expansion of bodies by heat—Cold by evaporation—Con-
ducting powers of different substances—To break glass in
any direction by heat—Cooling power of wire gauze—Dr.
Franklin's experiment on heat of colored cloths—To break
a roll of sulphurw y the heat of the hand—Prince Rupert's
drops—Reflection on heat—Formation of dew—Water
boiled by being cooled—Production of freezing mixtures—
Condensation of steam—Brightness of flame—To prove
that flame is hollow—How a candle burns—Oxygen ne-
cessary for combustion—Requisites to produce a flame—
Intense and rapid combustion—Detonation with sulphur
and chlorate of potass—Vivid combustion under water—
Detonation of chlorate of potass.
To sum up what has been stated above, the stu-
dent will bear in mind the following principles,
which the experiments will illustrate:—That
heat exists in two distinct states—as sensible heat
and as latent heat; that it may be procured, both
naturally and artificially, by the methods which
have been described; that it has a tendency to in-
crease the bulk of all bodies it combines with,
and diminish the bulk of those it separates from ;
and that it is constantly passing from one body to
another, endeavoring to restore an equilibrium by
the means just enumerated.
SENSATIONS OF HEAT DECEPTIVE.
275. If we place one of our hands in a basin
of hot water, and the other in a basin of cold wa-
ter, and then immerse both of them in another
basin containing luke-warm water, we shall feel
it to be cold to the hand that had been placed in
the hot water, and hot to that which had been
immersed in the cold. Our sensations of heat
are very apt to deceive us.
276. Two travelers arriving at a spot half way up
a mountain, will feel the temperature of the place
to be hot or cold, according to the warmth of the
place they have each of them left. The man as-
cending the mountain will feel cold, because the
higher we ascend in the air the colder it is; while
the traveler descending will feel warmer, for
the same reason. Thus, any particular part of a
mountain may appear agreeably warm to one
man, and intensely cold to another.
LATENT HEAT.
277. A quantity of heat exists in all bodies in
what is termed a latent state; that is, it cannot
be felt by the touch (see Introduction, 263). The
following experiments will, however, illustrate the
fact better than any description can.
278. Hammer a piece of cold iron for a short
time, and it will become exceedingly hot; if
hammered briskly on an anvil, it may be made
red-hot.
279. Rub a common brass coat-button, for a
short time on a piece of wood ; on applying it to
the hand, it will be found to have acquired a
high degree of temperature.
LATENT HEAT IN IRON.
280. The quantity of heat which exists, in a
latent state, in iron, may easily be shown by the
common flint and steel of a tinder-box. On strik-
ing the steel sharply with the flint, a portion of
the latent heat of the former is given out, suffi-
cient to melt a particle of the iron, and render it
red-hot. If the flint and steel be struck sharply
together, several times, over a clean sheet of writ-
ing-paper, a number of black spots will be found
on it, which are the particles of steel that have
been melted, and fallen on the paper.
LATENT HEAT IN WATER.
281. Water contains much heat, in a latent
state; and if we could compress it with the same
ease that we can many other, bodies, we might
squeeze this heat out, and render it sensible to our
touch. The same effect, however, may be pro-
duced in another way. Pour about a wine-glass-
ful of sulphuric acid (common oil of vitriol) into
a Florence flask, or other thin glass bottle, that
will, therefore, bear a sudden degree of'heat
without breaking ; into the flask pour about
twice or three times the quantity of wa- a
ter, and in a few minutes, although both B
the liquids were cold when mixed, a very B
great degree -of heat will become sensible. I\
Indeed, if the flask be immersed in wa./ \
ter, a sufficient degree of heat may be ob-i. j§
tained, by this means, to make it boil__J^f
Phosphorus may also be very easily ignited by Us
Philosophical Experiments. 77
The cause of this effect is believed to be as fol-
lows :—The sulphuric acid has a very strong af-
finity for water, and combines with it so inti-
mately, that the liquids, when mixed together, do
not measure so much as the sum of their meas-
ure when separate. Thus, a pint of sulphuric
acid, mixed with a pint of water, would not fill
a quart measure. It is evident, therefore, as the
liquids have decreased in bulk, a portion of the
latent heat that belonged to them must be given
out in their changing to a more solid state; and
this is the result that is produced. Care must be
taken, in making the experiment, to hold the
Florence flask so that, if it breaks with the heat,
the mixture within it shall not fall on the clothes
or furniture, as, otherwise, they will be much in-
jured. Thin glass vessels bear a sudden degree
of heat much better than thick ones, and a Flor-
ence flask is, therefore, well adapted for the ex-
periment.
LATENT HEAT IN A COMMON BUTTON.
282. If we take a common brass button, and
rub it smartly for a few minutes on the floor, or
against a piece of wood, it will become hot enough
to ignite phosphorus. At school, boys are prac-
tical philosophers when they perform this experi-
ment, and illustrate its effects, by placing the hot
button against the hands of their companions.
who may not be aware of the effects of friction
in developing latent heat.
LATENT HEAT DEVELOPED BY FRICTION.
283. Friction is one of the modes of procuring
artificial heat; and savages are said to procure
fire through its means alone (see Introduction).
If two pieces of dry wood be rubbed together for
for some time, they become heated; and if the
friction is continued, they may be made to in
flame. Large tracts of forests have frequently
been set on fire by these means in winter time,
when the boughs, being dry, the agitation of them
against each other, by high winds, produce suf-
ficient heat to ignite them. Sir Humphrey Da-
vy even obtained heat from ice, by friction : he
rubbed two pieces together in vacuo, and the la-
tent heat developed by this means was sufficient
to melt a portion of the ice. The effect of fric-
tion, in producing heat, is seen when a coach is
going down a hill, with the " skid" on one of the
wheels: sometimes the heat produced is so great,
that it has been known to set the wheel on fire.—
Great care is taken in constructing machinery to
provide against friction; not merely because it
impedes the action of the machine, but also to
prevent the heat that would otherwise be pro-
duced, which might prove of serious injury. The
experiment (282) with a common button is a
good example of the effects of friction in produc
ing heat.
LATENT HEAT IN THE AIR.
281. To exhibi' this, an instrument is sold at
the philosophical instrument-makers, called an
air syringe, or " the philosopher's tinder-box;"
but the same effect may be produced by a com-
mon popgun, which it very much resembles.—
Stop up the end of a popgun with wax, or some
other substance, so securely, that no air can es-
cape, and make the rammer to fit the tube as
tightly as possible, by greasing it. If a piece of
tinder be then placed in a little hole, which must be
made at the end of the rammer, and it is driven
down quickly, and withdrawn again into the air,
the tinder will be ignited. This is caused by the
heat that is given out on the sudden compression
of the air in the tube ; and if the apparatus is
made air-tight, a light may be produced by this
means much easier than by a flint and steel (see
Introduction). Although a popgun will do, a
metal tube, stopped at one end with a piston, to
fit air-tight, is better.
PPRODUCTION OF HEAT BY PERCUSSION.
285. The experiment (280) with the flint and
steel is an example of the development of heat,
by what is termed percussion, or the sudden
striking together of two bodies. Blacksmiths
frequently employ another plan to light their fires.
If a piece of iron be laid upon an anvil, and
Btruck sharply with a hammer for some time, it
may be made red-hot; the hammering causing
the iron to give out nearly all its latent heat.—
The effect may be shown by merely beating a
common nail with a hammer for some time, when
it will become warm enough to ignite a piece of
phosphorus; but if we wish to light a match by
this means, we must use a large piece of iron,
and beat it upon an anvil, or something similar.
The use of the latent heat in the iron, which is
forced out by this means, was to make it mallea-
ble and ductile, both of which properties it loBes
when its latent heat is forced out.
EXPANSION OF BODIES BY HEAT.
286. Measure a bar of iron, and afterward
place it in a fire till it becomes red-hot, when it
will be found, on again be-
ing measured while in that
state, to have increased in
length. When it coolr, it
will be of the same length
that it was before being ex-
posed to the fire (see Intro-
duction). The annexed cut
represents the iron rod and
measure by which this ex-
periment is generally performed.
287. Fill a phial with spirits of wine, and then
immerse it, nearly to the mouth, in hot water.__
The heat will expand the alcohol so much, that
it will run over the sides of the phial. When it
is taken out of the hot water, and cooled, the
quantity that has been forced out wdl be seen by
noticing how much would then be required to fill
the bottle.
COLD BY EVAPORATION,
288. Evaporation produces cold, because a
fluid, when it assumes the form of vapor, ab-
stracts a portion of heat from the body from
which it evaporates (see Introduction). To prove
this, place a small quantity of ether on the back
of the hand, and as it evaporates, considerable
cold will be felt. When persons catch cold after
getting their clothes wet, it is in consequence of
the evaporation of water cooling the body so
much, that the blood-vessels of the skin are una-
ble to perform their accustomed functions. This
is the reason why it is always important to put
off wet clothing as soon as possible, and to keep
78 Philosophical Experiments.
up the heat of the body by some stimulating
drink, or, what is better, by exercise.
CONDUCTING POWERS OF DIFFERENT SUBSTANCES.
289. Some substances will allow heat to pass
through them much easier than others. The for-
mer are called good conductors; the latter, bad.
If we place a piece of thick iron wire in the fire,
it will soon become so hot that we cannot hold it;
but if we use a piece of glass, we shall find that
we can handle it without inconvenience, even
when one end is intensely heated. In this case,
the iron is a good conductor, while the glass is a
very bad one. Advantage is taken of this cir-
cumstance in manufacturing many domestic ar-
ticles—for instance, the handle of metal teapots
is made of wood, because, otherwise, the hand
would not be able to bear the heat that would be
conducted to it.
TO BREAK GLASS IN ANY DIRECTION BY HEAT.
290. Glass being a bad conductor of heat, ad-
vantage may be taken of the circumstance to
break a piece in any direction, as follows:—Dip
a piece of worsted thread into spirit of turpen-
tine, and put it round the glass, in the direction
required to be broken; then set fire to the thread,
and the glass will crack exactly in a line with it.
A piece of red-hot iron ma}' be used for the same
purpose, but the effect can be produced more easi-
ly with the worsted.
COOLING POWER OF WIRE GAUZE.
291. If a piece of wire gauze be held in the
flame of a candle, it will be seen that the flame
will not pass through it. This is in consequence
Tof the metal conducting away the heat
so rapidly from the gaseous tallow, in
passing through, that when it reaches
the other side, it is not sufficiently hot to
combine oxygen, and therefore passes
away in the form of smoke. That such
is the case, may be proved by applying
a light to the smoke, which will then
ignite, and burn like the flame beneath.
292. The safety-lamp of Sir Humphrey Davy
was the result of his discovery of the cooling
powers of wire gauze. Before this lamp was in-
vented, the men employed in coal mines were
exposed to great danger, in consequence of the
frequent explosions that took place when a stream
of explosive gas, called fire-damp, came in con-
tact with their candles. This gas, which very
much resembles the common gas used in our
shops, is very explosive when mixed with air, and
is formed in fissures in coal in the mines. It fre-
quently happened, therefore, that when a miner
was at work, he liberated a quantity of this gas,
which, mixing with the atmosphere around, be-
came as explosive and destructive as gunpowder;
and when it came in contact with a light, its ef-
fects were as destructive. Accidents were so
frequently occurring, and so many men were kill-
ed, that at last a society was formed, to endeavor
to find out some means of preventing them ; but
their efforts were unsuccessful. At length they
applied to Sir Humphrey Davey, who, on experi-
menting on the gas, discovered that it would not
explode unless it came it contact with flame; and
he thought that if, therefore, a light could be en-
closed, so that while a sufficient quantity of air
should be supplied to it to keep it burning, the
flame should be prevented communicating with
the air without, that a perfect safety lamp
would be provided for the miner. After a varie-
J3^ ty of experiments, he constructed
iJL one similar to that represented in
|ijij7 the accompanying wood-cut. It
lip represents a common lamp, sur-
H rounded with a ehicld of iron
IB wire gauze, which has the same
\W\ effect in extinguishing flame,
|§| when it endeavors to pass through,
|3 as a piece of gauze has with a
|H candle. When, therefore, the mi-
ifij | ner, with his lamp, is suddenly
IB surrounded with a quantity of ex-
|nl plosive gas, he is no longer in
3& danger; because the flame of the
=jffij[glamp cannot pass through the
a|H§? gauze to explode the gas. So
^0* effectual, indeed, is this simple
piece of apparatus, that it is found, even when
the gauze becomes red-hot from the quantity of
explosive gas burning within the lamp, that it
will not explode that on the outside. And from
a knowledge of the simple property of wire gauze,
which any one may illustrate with a candle, the
philosopher has been enabled to construct an in-
strument which has been the means of saving
the lives of thousands.
DR. FRANKLIN'S EXPERIMENT ON HEAT OF COLORED
CLOTHS.
293. On a winter's day, when the ground is
covered with snow, take four pieces of woolen
cloth, of equal dimensions, but of different col-
ors—viz. black, blue, brown, and white, and lay
them on the surface of the snow, in the imme-
diate neighborhood of each other. In a few hours
the black will have sunk considerably below the
surface; the blue almost as much; the brown
evidently less; while the white will remain near-
ly even on the surface. Thus, it appears that the
sun's rays are absorbed, and conducted through
them to the snow, much more rapidly than by the
other colors. And it is, perhaps, for this reason,
that dark-colored clothes are preferred in winter,
while lighter ones are considered more suitable
for summer.
TO BREAK A ROLL OF SULPHUR BY THE HEAT OF THE
HAND.
294. Sulphur is a very bad conductor of heat.
If a roll of it be held in the warm hand for a few
minutes, it will snap, and break into two or more
pieces. If it be held over the flame of a lamp,
it will crumble, and separate still more. Break-
ing a roll of sulphur, by the mere heat of the
hand, is a very pleasing illustration of the effects
of heat.
prince rupert's drops.
295. The little glass toys, known by this name,
may be purchased at any glassblower's, for about
sixpence a dozen; and they illustrate, in a very
striking manner, the effects of heat on bad con-
ductors. Glass is a bad conductor, and this is
a cause of its being frequently broken. If hot
water, is poured suddenly into a tumbler, the in-
terior expands before the heat can affect the out.
side, and it therefore tears the particles on the
Philosophical. Experiments.
79
outside from each other ; in other words, it cracks
the glass. This is the reason why it is necessary
to have retorts, and other kinds of chemical ap-
paratus, intended to be exposed to much heat,
made very thin, in order that the heat may pass
readily through them. Prince Rupert's drops are
lumps of glass, let fall, while melted, into water,
and are thereby suddenly cooled and solidified on
the outside, before the internal part is changed;
then as this at last hardens, and would contract,
it is kept extended by the arch of external crust
to which it adheres. Now, if a portion of the
neck of the lump be broken off, or if other vio-
lence be done, which jars its substance, the co-
hesion is destroyed, and the whole crumbles to
dust, with a kind of explosion. Any glass cool-
ed suddenly when made, remains very brittle, for
the reason now stated. What is called the Bo-
logna jar, is a very thick, small bottle, thus pre-
pared, which bursts by a grain of sand falling
into it. The process of annealing, to render
glass-ware more tough and durable, is merely the
allowing it to cool very slowly, by placing it in an
oven, where the temperature is caused to fall
gradually.
REFLECTION OF HEAT.
296. Bright substances reflect heat much bet-
ter than dark and rough ones, which absorb it
best. If a piece of tin be held before the fire, it
will take some time before it becomes hot, be-
cause it reflects the light and heat; but if it be
covered with lamp-black, it wdl soon become
heated. Meat-screens for our kitchen fires are
formed on this principle: they reflect the heat on
to the roasting meat.
FORMATION OF DEW.
297. Dew is deposited on the leaves of plants,
in consequence of their giving out so great a
quantity of heat, by radiation, on clear, bright
nights, when there are no clouds, that the tempe-
rature of the plant is reduced below that of the
atmosphere. When this takes place, the heat of
the atmosphere is absorbed by the plant, and is,
consequently, unable to retain so great a quantity
of moisture; warm air possessing the power of
holding more vapor in it than cold air. The
manner in which dew is deposited on plants may
be seen, by bringing a glass of cold water from a
well into a warm room. The cold water absorbs
some of the heat of the surrounding air, which,
in passing through the sides of the glass, leaves
behind the water it contained in a state of vapor :
tliis will be seen on the glass. Water decanters
show this in summer.
WATER BOILED BY BEING COOLED.
298. Water boils, on the surface of the earth,
at a temperature of 212 degrees; but on the tops
of high mountains, where the weight of the at-
mosphere is somewhat less, the boding point is
lswer than 212 degrees. To prove that the pres-
sure of the atmosphere has great influence over
the boiling point, the following striking experi-
ment can be performed :—Fill a Florence flask
about half full of water, and then expose it to the
heat of a spirit-lamp until it boils ; when this
takes place, put a cork in the flask, and remove it
from the lamp, when the steam wdl be condensed.
In a very short time, however, if the bottle has
been corked tightly, so that the air cannot enter
when the steam is condensed, the water will be-
gin to boil again; and if the flask is placed in cold
water, the boding will be stdl more violent. If
the flask be then removed from the cold water,
and placed in hot water, the boiling will cease. ^
The cause of this, apparent anomaly is, that
when the flask is placed in cold water, the steam
or vapor in the bottle is condensed; and there be-
ing, therefore, little or no pressure on the surface
of the water, the air having been expelled by the
steam, the heat contained in the water is sufficient
to cause it to boil, and the additional heat im-
parted to it by the hot water makes it bod rapidly.
When the flask is placed in the hot water, a vapor
is formed, which presses on the surface, similar
to the atmosphere; and, consequently, prevents
the liquid boding, except at a higher temperature.
Water will bod at 90 degrees in vacuo, and when
the steam is condensed in the flask, there is a very
good vacuum formed above the water; so that,
indeed, the warmth of the hand is then almost
sufficient to make the wa£er boil.
PRODUCTION OF FREEZING MIXTURES.
299. Liquids, when they become more dense,
or solid, give out heat (as in experiment 281;)
solids, when they are rendered fluid, without the
application of heat, become very cold. Advan-
tage is taken of this circumstance to produce
what are termed frigorific mixtures. The follow-
ing may be formed, without much trouble, and
will illustrate the fact very well.
300. Mix two parts of snow, or pounded ice,
with one of common salt. The mixture soon be-
comes liquid, and the temperature falls 41 degrees
below the freezing point of water. To produce
this effect, a quantity of the materials must be
used. From a knowledge of the effects of salt
upon ice, it is frequently used, during a frost, to
melt the ice upon the pavement, &c.
301. Mix sixteen parts of water with five of
nitre, and five of sal ammoniac, in fine powder,
when the temperature will fall about 40 degrees
below the freezing point. The former experiment
can only be conveniently performed in the winter;
but this can be produced at any time.
CONDENSATION OF STEAM.
302. Water, when exposed to a heat of 212
degrees, is formed into steam. In this state, the
particles that compose water are so far separated
by heat, that it is found steam occupies the 1,700th
space of an equal weight of water. When, how-
ever, the heat is abstracted, the steam is con-
densed into the original quantity of water from
which it was formed. To prove this, procure a
Florence od-flask, and bod a small quantity of
water in it; when the steam is issuing from the
mouth, put in a cork, having previously covered
the hand with a towel, to prevent the steam scald.
ing the hand. If the flask be now placed in cold
water, and the cork taken out, the steam will be
condensed, and the water will rush into the bottle,
and completely fill it. This is sometimes effected
with so much force, that the flask is driven out
of the hand, and even broken ; care must, there-
fore, be used in performing the experiment.
BRIGHTNESS OF FLAME.
303. The brightness of a flame depends upon
SO Philosophical Experiments.
the quantity of oxygen it receives, as may be
shown by a common candle. If we examine the
flame, we shall perceive, that on the outside it is
bright, while there is a cone, of a dark color, in
the centre : this part, indeed, is not a light, as
may be proved by holding a clean card, for a
minute, in the centre of a flame ; on withdrawing
it, there will be found a dark circle—showing
that it was only the outer portion of the flame, in
contact with the air, that was capable of burning
the card. If all the tallow were consumed, there
would be no smoke; for smoke is the particles of
tallow, passing off in an unconsumed state. In
the common lamps, used by butchers, the waste
in this way is very great; and before the intro-
duction of the Argand burner for lamps, this was
an evil that could not be remedied. The inventor
of this burner considered, as the brightness of a
flame, and the complete combustion of the ma-
terial, depended upon the supply of oxygen, that
if, instead of having the wick of a lamp in a
solid piece, like the wick of a candle, it were
made hollow, or so that it might be placed round
a hollow cylinder, the, r»mbustion would be more
perfect. He accordingly constructed a lamp,
with a burner of this kind, and the effect he an-
ticipated was produced: at the same time, he
found that, by using a glass cylinder, similar to
the common gas-glasses, that the draft was pro-
moted, and a greater supply of oxygen afforded
to the flame. This invention has since been uni-
versally adopted; and gas-burners are constructed.
on a similar principle. In lamps, the wick, which
is hollow, is placed round a brass tube, and can
be raised, or dressed, at pleasure; the lower end
is placed in oil, which it absorbs, and brings
gradually in contact with the flame ; a glass is
placed round this, and air is supplied to the inte-
rior of the flame through the tube, and to the ex-
terior in the ordinary way.
HOW A CANDLE BURNS.
304. The combustion of a candle (see Intro-
duction) illustrates many natural laws in a sim-
ple manner. When the wick is lighted, it melts
a portion of the tallow immediately beneath, and
forms a little cup, in which a quantity of the li-
quid tallow continues. The wick, by capillary
attraction, draws up a portion of this tallow,
which enters the flame. Here it becomes a gas,
and combines with the oxygen of the atmosphere,
j. forming carbonic acid. A
-^£ portion of the gas formed
«Mg^ from the melted tallow
'^k^^l&k^ )l may be ignited away from
^|% ^^feinfiL the candle, by placing a
' ^S&l^ sma" time> rather wider
^a£r than the bore of a piece of
tobacco-pipe, in the dark
part of the flame: the gas
fwill pass through this, and
if a light be applied at the
other end, it may be igni-
ted. The existence of the
carbonic acid may also be shown by holding a
lighted match a little above the candle, when the
former will be extinguished.
305. The benefit of the Argand burner wdl be
seen immediately, if we place a card at the bot
torn of the tube, so as to stop the supply of airt^
the interior of the flame. The consequence wil
be, that much of the oil will be unconsumed, and
the lamp will give off a great deal of smoke.
TO PROVE THAT FLAME IS HOLLOW.
306. Drop, carefully, some spirits of wine on
the surface of water, within a small hoop, float-
ing in a large basin ; set the spirits on fire, and
then introduce the finger under the edge of the
hoop, and up through the water, into the interior
of the flame. If this be done carefully, no heat
will be felt, except the finger is raised sufficiently
high to touch the film of flame itself.
REQUISITES TO PRODUCE FLAME.
310. There are several requisites for the pro-
duction of a flame, and without which, it can-
not exist. The first is, that oxygen must be pre-
OXYGEN NECESSARY FOR COMBUSTION.
307. Put a little water in a soup-plate, and on
it place a piece of wax taper, or candle lighted,
so that it may swim on the surface; then take a
common beer tumbler, and cover the taper over
with it: the consequence wfll be, that, after a
short time, the light will be extinguished, and
the water from the plate will rise a little way in
the tumbler. This experiment shows the neces-
sity of oxygen in combustion ; for directly the
light had absorbed all of it that was contained in
the air under the glass, it went out. The rising
of the water is in colrsequence, principally, of the
cooling of the air again within the tumbler;
while it was heated, a portion was driven out,
and on cooling, the water supplies its place, be-
ing forced in by the pressure of the air on the
outside.
308. Another experiment, illustrating the
same fact, may be performed in the following
way:—Take a large wide-mouthed bottle, with
the bottom broken off, and place it a httle way in
a pail of water; then hold the nostrils close with
one hand, and breathe the air in the bottle sever-
al times. By this means, the greater portion of
the oxygen contained in the air m the bottle will
be absorbed, as we all abstract oxygen from the
air every time we breathe. When the mouth
is withdrawn from the mouth of the bottle, place
the hand over it, and get a person to introduce
into it a lighted match, which, it will be seen, is
instantly extinguished. Instead of using a bot-
tle, a better piece of apparatus is a common gas-
receiver.
The rationale of both these experiments is
nearly the same. In the first, the burning taper
absorbsMhe oxygen, and forms carbonic acid gas:
in the second, a similar effect is produced by the
carbonaceous matter of the blood uniting with
the air in the bottle, and forming the same gas.
This gas will neither support life nor flame: and
if, therefore, a living animal, or a light, be intro-
duced, the first should be killed, and the latter ex-
tinguished.
310. The use of the bellows, in making a fire
burn brighter, is simply because they force a
greater quantity of air, and consequently, more
oxygen, against the burning material than it
would otherwise receive. The damper of a
chimney produces an effect precisely opposite, by
lessening the supply of air sent to the fire.
Philosophical Experiments. 81
sent, in some form, to support combustion; and
the second, that the body must be heated to a
high degree of temperature. There is one excep-
tion to the first of these requisites, since bodies
will burn in chlorine gas, which it has been pro-
ved does not contain oxygen.
311. Flame is the intensely heated particles of
a burning body, in the act of umting with oxygen.
Thus, in the case of a common lamp, the oil is
absorbed by the wick, and the particles, when
they enter the flame, become white-hot, and then
pass off as a gas. Experiment 308 will show
the necessity for oxygen to support combustion ;
and it is, therefore, only necessary to prove, that
whatever lowers the temperature of a burning
body destroys-flame.
312. Get a piece of wax candle, and pull
all the wick out except one thread, so that,
when this is lighted, the flame shall be very
small. Then make a little ring of iron wire,
about the eighth of an inch in diameter,
which affix to a handle. It will be found
that if, when the wick is lighted, this wire ring is
passed over, so as to go below the flame, that it
will be immediately extinguished. This is in
consequence of the iron wire being a good conduc-
tor, ahd, therefore, the heat of the flame is carri-
ed awa>j so quickly by it, that the wax cannot
become white-hot, and unite with the oxygen of
the atmosphere; the flame is, therefore, extin-
guished. The was, in a gaseous state, will not
combine with the oxygen, unless at a high degree
of temperature ; and it is evident, therefore, that
anything which cools the wax must prevent the
combination taking place.
313. A similar effect to that produced by the
cold ring of wire may be shown, by merely bring-
ing a penny piece, or other good metafile conduc-
tor, in contact with the flame. When the candle
has been extinguished by this means, ligkt it
again, and make the ring of wire hot; then passit
again over the flame, and it will not put it out.—
This shows, satisfactorily, that, in the former in-
stance, the effect was produced simply in conse-
quence of the rapid absorption of the heat by the
• metal.
INTENSE AND RAPID COMBUSTION.
314. To illustrate the sudden combustion of
bodies, through* intense chemical action, the fol-
lowing experiment may be performed ?—Mix a
little chlorate of potass, about the siz"£ j&a. pea,
with the same quantity of loaf sugar, having
previously reduced them each to powder. Place
the mixture on a piece of tile, or iron, and dip a
glass rod into a bottle of sulphuric acid ; let the
acid from the rod drop upon the mixture of chlo-
rate of potass and sugar, and they wdl imme-
diately flame.
Care must be taken in making this experiment,
not to use a large quantity of the materials em-
T H E
ployed : the effect will be produced as well with
the quantity we have mentioned, as if it were
twenty times as great, and there is no danger at-
tending the experiment; but if a large quantity
be used, the matter will perhaps fly about, and
might occasion injury. The face must be kept
from the mixture when the sulphuric acid is
dropped into it, as it bursts into flame almost in-
stantly.
The rationale of the experiment is, that the
chlorate of potass and the sulphuric acid have a
powerful affinity for each other, and when they
come in contact, they combine with great in-
tensity ; -much heat is, therefore, given out—suf-
ficient to ignite the materials. The loaf sugar is
used, becaaa^feircbuiBis readily, and thus affords
material for the potass and acid to act upon: that
this is its only use, may be seen by mixing some
of the chlorate of potass with sulphuric acid by
themselves, when the effect, will more resemble an
explosion than the combustion that ensues in the
former instance.
315. If equal parts of chlorate of potass and
camphor, mixed togethejAe touched with a drop
or two of sulphuric ac^^the camphor will in-
flame. The same effect takes place with spirits
of wine, or charcoal, instead of camphor.
These experiments must be conducted with
care.
DETONATION WITH SULPHUR AND CHLORATE OF
POTASS.
316. Into a mortar put two or three grains of
chlorate of potass; and after having reduced it to
powder with the pestle, introduce some flour of
sulphur, or brimstone, very finely powdered. If
the two be now rubbed together, they will be de-
tonated, with a smart noise, like the cracking of a
whip ; and this may be repeated a dozen times,
with the same quantity of materials. This is a
very pleasing experiment, quite unattended with
danger of any kind.
VIVID COMBUSTION UNDER WATER.
317. Place a small piece of phosphorus, and a
few grains of chlorate of potass, in a tumbler, or
other vessel, and pour on them, gently, some hot
water. Tins will inflame the phosphorus, and its
combustion, being supported by the chlorate of
potass, a very pleasing and vivid light will be wit-
nessed under the water.
318. If a little oil be placed on the top of the
water in the vessel, it will be inflamed.
DETONATION OF CHLORATE OF POTASS.
319. Many substances, when heated to a cer-
tain degree of heat, change their form, with an
explosion. If a little chlorate of potass be put
on a fire-shovel, and placed over the fire, when
the shovel has received a certain heat, the chem-
ical detonates, with a sharp report.
•
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