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ON PHYSICS, OR NATURAL PHILOSOPHY.

No. LIX.

(Continued from page 494.)

that is to say, bring it back to the natural state in two ways, by a slow or an instantaneous discharge. To discharge it slowly, first touch the plate A-that is, the plate which contains an excess of electricity-with the finger, then all the positive fluid which is not made latent by the negative fluid of the

EFFECTS PRODUCED BY THE ACCUMULATION OF disc c escapes to the earth, and as the disc c only renders

BOTH ELECTRICITIES.

Latent Electricity; Condenser.-Latent electricity is the state of neutralisation presented by the two electric fluids when, being brought together on the surfaces of two conducting bodies, they are separated by only a thin non-conducting layer. Through this neutralisation the electric charge may become very considerable, and greatly surpass what would take place in a single body. The apparatus by which electricity is thus accumulated is called a condenser. There are various sorts of condensers, all based upon the principle of electrisation by influence, and consisting of two conducting bodies separated by a non-conducting body.

399.

The condenser of Epinus is formed of two circular copper plates ▲ and c, and a glass plate в which separates them, fig. These plates being each furnished with an electric pendulum having a conducting rod, are isolated by glass feet, capable of sliding along a groove in the stand upon which they are placed. They are thus brought near to each other or separated to any distance that may be required. To collect the two electricities on the copper plates, put them in contact with the glass plate, as in fig. 398, then by means of

Fig. 398.

latent a quantity of electricity less than its own, it is the plate c which after this first contact possesses the strongest charge; in fact, we see that the pendulum a falls back and the pendulum c diverges. If we now touch the disc c, its pendulum falls back while the pendulum a diverges, and so on if we continue touching the two discs alternately. The discharge takes place only very slowly, and if the air is dry, it is not completed until several hours have elapsed. If you first touched the plate c, which is less electrised, you would not remove any electricity from it, because all that it contains is rendered latent by the disc A.

When we wish to discharge the conductor instantaneously, we bring the two plates into communication by means of the exciter, an instrument consisting of two brass arcs with a ball of the same metal at the end of each, and connected together by a hinge upon which they turn. When the instrument is furnished with glass isolating handles, as in fig. 400, it is called the glass-handled exciter; if there are no handles, it is called the simple exciter. To make use of the exciter, apply one of the balls to one of the plates of the condenser, and bring the other near the second plate. A strong spark then appears, arising from the recombination of the contrary electricities Fig. 399.

metallic chains make one of them, as e. g. A, communicate with an electrical machine and the other with the earth. The disc A is then electrised positively, like the machine, and if it were alone it would have the same quantity of electricity on an equal surface, allowing for the influence of the form; but the disc c completely changes the phenomenon, and it is that which causes the accumulation of the two electricities. In fact, the positive fluid of the disc a acting by influence through the glass on the plate c, attracts the negative fluid and repels the positive fluid into the earth. Now the negative fluid of the disc c reacts in its turn upon the positive fluid of the disc A and neutralises it, but only partially, on account of the interval between them. The electric tension on the disc A is no longer in equilibrium with the tension of the machine: the consequence of which is, that this latter communicates to the plate a fresh quantity of positive fluid, which acts as before upon the disc c, and so on up to a certain limit.

Slow and Instantaneous Discharge.-When the condenser is charged, that is to say, when the contrary electricities are accumulated on the two surfaces, the communication with the electrical machine and with the ground is broken by removing the two metallic chains. Only a part of the electricity of the plate A is then latent, while that of c is completely so. In fact the pendulum a diverges, while the pendulum c is vertical. But if we remove the plates from each other, fig. 399, both pendulums diverge, for the electricities are no longer latent. The plates being in contact with the isolating plate, fig. 398, and the chains removed, we may discharge the condenser,

VOL. V.

accumulated on the two surfaces of the condenser. The recombination, however, is not complete, for we may in the same manner elicit a second and a third spark, and even more, though they become more and more feeble. Hence it is inferred, that when the two plates communicate together, the two electricities cannot be entirely recombined. On discharging the condenser with the exciter, we feel no sensation though we hold the exciter in the hand, and though it be the simple exciter. This

Fig. 400.

is owing to the fact, that the electric fluid always choosing electricities is effected by the metallic arc, and not by the body of the experimenter. But if, while touching one of the

the best of two conductors, the recombination of the two

137

surfaces with one hand, you bring the other near the second surface, the recombination will take place through the arms and body, and a shock will be experienced, the violence of which will be proportional to the size of the surface of the condenser and the strength of the electric charge.

Volta's Condensing Electrometer.This is nothing else than the gold-leaf electrometer already described, with the addition of two condensing disos. The copper rod which bears the pieces of gold leaf, instead of terminating above in a brass ball, ends in a brass disc, on which is placed a piece of glazed taffeta, fig. 401, rather larger than the disc, and serving to isolate it from a second disc of a similar sort, but furnished with a glass handle and placed above it. To render even small quantities of electricities perceptible by this electrometer, bring the body whose amount of electricity you wish to determine into communication with one of the plates, which is then called the collecting plate, and the other plate in communication with the earth, by touching it with the finger slightly wetted, fig. 402. The electricity of the body on which you are experi

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other, but one of them communicates with the frame by means of a small piece of tin which bends over at A, fig. 403, in such

Fig. 403,

a manner that it touches the thumb of the person who holds the instrument in his hand. To charge the fulminating square, bring the isolated tin-foil-that is, the tin-foil which does not communicate with the wooden frame-near an electrical machine. As the other sheet of tin-foil is brought into communication with the earth by the hand, the two sheets act exactly like the plates of the condenser of Epinus, and a great quantity of contrary electricities is collected on the two surfaces.

The fulminating square, like the condenser, is discharged with the simple exciter. For this purpose, hold the square in the hand, and apply one of the balls of the exciter to the extremity A of the little strip of tin belonging to the lower tin-foil. Then turning the exciter on its hinges, bring the other ball near the upper tin-foil, when a bright spark will appear accompanied by a report, owing to the recombination of the two electricities; but the experimenter will feel no shock, because the recombination takes place entirely through the metallic exciter. If, on the contrary, while holding the apparatus in the same manner, you first touch the isolated tin-foil, you will experience a violent shock, as the recombination will take place through the arms and body,

menting then spreads over the surface of the collecting plate, and acts through the taffeta on the second plate and on the hand, so as to repel the electricity of the same kind to the earth and attract that of a contrary sort. The two fluids therefore collect on the two plates just as in the condenser of Epinus, but without any divergence in the pieces of gold leaf, since the two electricities are rendered latent. The apparatus being thus charged, you may first withdraw your finger, and then the source of electricity, without as yet observing any divergence. But if you take up the upper plate, fig. 401, the electricity is no longer latent, and that of the second plate being distributed equally over the rod and over the pieces of gold leaf, these diverge very much. The divergence may be greatly increased by fitting to the foot of the apparatus two copper rods terminating in balls of the same metal, for these balls being electrised by the influence of the pieces of gold leaf, react upon them. The sensibility of the apparatus may be still further increased by removing the taffeta and separating the two plates by nothing more than a very thin layer of gum-lac varnish upon them. Lastly, instead of taking the upper plate for the collecter, as in our figure, it is better to take the lower plate, because it is always the plate which commuticates with the source that is most charged. Like all electric paratus, the condensing electrometer requires to be carefully Iried and even warmed before experimenting.

The Fulminating Square is a condenser more simple than that f Epinus, and better adapted to produce lively sparks and violent shocks. It consists of an ordinary square of glass with a wooden frame round it. On the two surfaces of the glass are stuck two leaves of tin-fail opposite each other, and leaving border of about two inches between each and the frame all round. The leaves of tin-foil do not communicate with each

The Leyden Jar, so-called from the place where it was invented, is ascribable to Musschenbroeck, a Dutch philosopher (some say his pupil, Cuneus), who discovered it accidentally in 1746. Having fixed a metallic rod in the cork of a bottle full of water, he brought it near an electrical machine, intending to electrise the liquid. Now the hand which held the bottle performing the office of one of the plates of the condenser, while the water inside represented the other, positive fluid collected on the inner surface of the bottle, and negative fluid on the outer surface in contact with the hand. Consequently, having brought one hand near the metallic rod while the other grasped the bottle, Musschenbroeck_received so violent a shock that, as he afterwards wrote to Reaumur, he would not have it again for the whole kingdom of France. However, this experiment being once known, attempts were made in all quarters to repeat it. The abbé Nollet, professor of natural philosophy at Paris, first replaced the water in the bottle by crumpled sheets of tin-foil, copper, silver, or gold. An English philosopher had already discovered that, by covering the exterior with tin-foil, the shocks might be rendered much more violent. The Leyden jar then took the form it still retains, but the theory of it was not understood till Franklin explained it by showing that, like the fulminating square, it is really a condenser.

As represented in fig. 404, at the moment of discharge, the

Fig. 404.

Leyden jar consists of a thin glass bottle, varying in size according to the quantity of electricity which is required to be collected. The inside is filled with gold or copper leaf. The outside and the bottom are covered with tin-foil B, which, however, terminates at a considerable distance from the neck of the bottle. Through the cork passes a copper rod bent into a hook, and terminating in a knob A. Inside, this rod communicates with the gold or copper leaf which fills the bottle, and is called the internal armature, the tin-foil в being called the external armature.

The Leyden jar is charged, like the condenser of pinus and the fulminating square, by making one of the armatures communicate with the earth and the other with the electric source. For this purpose, hold it in the hand by the external armature, and present the internal armature to an electrical machine, the positive fluid then collects on the gold leaf, and the negative upon the tin-foil. The contrary would take place if, while holding the jar by the hook, you were to present the external armature to the machine. The theory of the Leyden jar is the same as that of the condenser. Like the condenser, it is discharged slowly or instantaneously. To discharge it instantaneously, hold it as in fig. 405, and bring the two

Fig. 405.

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armatures into communication by means of the simple exciter, taking care first to touch the armature held in the hand, otherwise a shock will be felt. To discharge it slowly, isolate it on a cake of resin, and touch, first the internal armature, with the finger or a metal rod, and then the external armature, and so on continually, eliciting each time a feeble spark. To render the slow discharge more perceptible, arrange the Leyden jar as represented in fig. 406. The rod is straight and furnished with a small bell. Near the jar is a metallic rod with a second bell like the first, and a small electric pendulum consisting of a copper ball attached to a silk thread. The jar not being fixed to the board в on which it is placed, take hold of it by the external armature and charge it by bringing it near an electrical machine, and then put it on the board. The internal armature now containing an excess of positive electricity not neutralised, the pendulum is attracted and knocks the bell of the jar. It is then repelled immediately, and goes to the second bell, to which it communicates its electricity. But on returning to a neutral state it is again attracted by the first bell, and so on for several hours, if the air is dry and the jar large.

which are capable of separation, consists of a large conical glass vessel B, fig. 407, an external armature c of tin plate, and an internal armature D of the same material. These portions being placed one in the other, as represented in fig. A, form a complete Leyden jar. After having electrised it, like the common jar, and isolated it on a cake of resin, fig. A, remove the internal armature with the hand, then the glass vessel, and lastly the external armature, and arrange them all in a row as represented in the figure. Now the two armatures are evidently thus brought to the natural state. But if you put back the armature c on the cake of resin, and put the glass vessel in it, and again the armature D in this, you again form a Leyden jar, which gives a spark almost as strong as if you had not discharged the two armatures. Hence we infer that the two latent electricities, yielding to their mutual attraction, leave the two armatures in a great measure and go to the surfaces of the glass.

Cascade Charge.-This name is given to an electric charge which is transmitted from one Leyden jar to another, when they are arranged one above another as follows. The first is attached by its hook to the conductor of an electrical machine, then the hook of the second passes through a metallic ring fastened to the external armature of the first; a third is attached to the second in the same manner, and so on to the number of five or six, the external armature of the last communicating with the earth by a metallic wire. As soon as the first jar is charged, it reacts upon the neutral fluid of the second and decomposes it, then this reacts in the same way upon the neutral fluid of the third, and so on throughout till all the jars have the same fluid as the machine, and the contrary at their external armatures. These jars can be discharged one after the other, or all together, by making the internal armature of the first communicate with the external armature of the last.

Fig. 407.

Electric Jars and Batteries.-An electric jar is a large Leyden

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jar with a neck wide enough to enable one to stick tin-foil all round the inside for the internal armature. The rod which goes through the cork is straight, and terminates below in a metallic chain, which puts it in communication with the tin-foil that forms the internal armature. A battery is a collection of several jars in a wooden box, fig. 408, communicating together, Fig. 408.

external armatures of the jars. The tin-foil also lines the sides of the box as far as the two metallic handles. The battery is charged, as seen in the figure, by bringing the internal armatures into communication with an electrical machine, and the external armatures with the ground by the wood of the box and the table on which it rests, or, still better, by a metallic chain attached to one of the metallic handles. An electrometer with a dial fixed to one of the jars, serves to indicate the charge of the battery. In spite of the large quantity of electricity collected in the apparatus, the electrometer diverges only slowly and a few degrees, which ought not to occasion surprise, since the divergence arises solely from the difference in the tension of the two armatures. The number of jars is generally four, six, or eight. The larger and more numerous they are, the more time is required to charge the battery. To discharge it, bring the two armatures into communication by means of the exciter, taking care to touch the external armature first. We must in this case use the glass-handled exciter, and take every precaution to avoid a shock, otherwise with a strong battery serious consequences might result. When we wish to strike down an animal, or any object whatever, we make use of the universal exciter represented in fig. 409. It is a small wooden box with two glass columns, on which copper rods are hinged. Between these columns is a glass support with a small plate, on which is placed the animal or object upon which we wish to experiment. The two copper rods being directed towards this object, one of them is made to communicate with the external armature of the battery, and the other with one of the balls of the glass-handled exciter. Then bringing the other ball of the exciter near the internal armature, a spark appears between this ball and the armature, and another between the branches of the universal exciter. It is the latter spark that strikes the object. Fig. 409.

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internally by means of metal rods, and externally by tin-foil which lines the bottom of the box, and is in contact with the

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is to consider habits and habitual actions as they partake of a moral character, or as they are the object of moral approbation or disapprobation. If we should remove from the list of moral actions all those which are prompted by habit, we should cut off the larger number of those which men have agreed in judging to be of a moral nature.

That there are virtuous habits and vicious habits, will scarcely be denied by any considerate person. A habit of lying, of swearing, of slandering, of cheating, of irreverence, of indolence, of vainglory, with many others, are, alas! too common. There are also virtuous habits, such as of industry, temperance, kindness, veracity, diligence, honesty, etc. To be sure, these virtues commonly flow from principle, but the practice of them is greatly facilitated by correct habits. Two considerations will show that men are properly accountable for those actions which proceed from habit. The first is, that in the formation of his habits man is voluntary. The acts by which they are formed are free acts, and the agent is responsible for all their consequences. The other consideration is, that habits may be counteracted and even changed by the force of virtuous resolutions and perseverance. Where habit has become inveterate, it may be difficult to oppose or eradicate it; but the strength of moral principle has often been found sufficient to counteract the most confirmed habits. When it is asserted that men long enslaved by evil habits cannot make a change, it is on the ground that no principle of sufficient power exists in the mind of the agent; but for that deficiency the man is responsible. Yet a power from without may introduce a new principle potent enough to overcome evil habits. The importance of possessing good habits is admitted by all moralists. Aristotle makes the essence of virtue to consist in "practical habits, voluntary in their origin," and agreeable to right reason. Dr. Thomas Reid, in his "Essay on the Active Powers," defines virtue to be "the fixed purpose to act according to a sense of duty," which definition Dugald Stewart modifies, by observing, "It is the fixed purpose to do what is right, which evidently constitutes what we call a virtuous disposition. But it appears to me that virtue, considered as an attribute of character, is more properly defined by the habit which the fixed purpose gradually forms than by the fixed purpose itself." Dr. Paley lays it down as an aphorism, that "mankind act more from habit than reflection." "We are," says he, "for the most part, determined at once, and by an impulse which has the effect and energy of a pre-established habit." To the objection, "If we are in so great a degree passive under our habits, where is the exercise of virtue, or the guilt of vice?" he answers, "in the forming and contracting of these habits." "And hence," says he, "results a rule of considerable importance, viz. that many things are to be done and abstained from solely for the sake of habit."

THE NATURE OF VIRTUE.

The theories on this subject have been numerous, and contrary to one another. It is now proposed to mention some of the principal of them. We shall first mention the theory of Mr. Hobbes and his followers, who deny that there is any natural distinction between virtue and vice, and maintain that by nature all actions are indifferent, and that our ideas and feelings on the subject of morality are altogether the effect of education and association. Mr. Hobbes did indeed maintain that men are bound to obey the civil government under which they may happen to live, and to conform to the religion established by law, however contrary to their own private judgment. All moral duty, according to this theory, was resolved into the authority of the law of the land. As no natural moral rule existed, it was held that, except so far as a man was restrained by civil authority, he had a right to do what he pleased; and while he confined himself within these bounds, he need feel no concern about the consequences of his conduct.

Perhaps the most extraordinary system of virtue every promulgated was that of Mandeville, who maintained that all pretensions to virtue were mere hypocrisy, which men assumed from the love of praise. This writer forgot that hypocrisy assumes it as true that that which is counterfeited is an object of esteem and approbation among men. That virtue consists in the mere pursuit of pleasure, or of our own interest, is a system as old as Epicurus, and has had many abettors up to this time.

But the whole plausibility of their arguments depends on the pre-established connexion between happiness and a virtuous course of life. That true happiness is the natural effect of virtue, falls entirely short of proving that the essence of virtue consists in the tendency of certain actions to the person's true interest; whereas, when we perceive an action to be virtuous, we are conscious that it is not from any view of the connexion of the action with our own happiness that we approve of it; but our judgment is immediate, founded on a moral character perceived in the act itself. And in many cases virtue requires us to deny ourselves personal gratification for the sake of others. A man supremely governed by a regard to his own interest, is never esteemed a virtuous man by the impartial judgment of mankind. According to this theory, the only thing censurable in the greatest crimes is, that the guilty person has mistaken the best method of promoting his own happiness. Upon this principle, a man is at liberty to pursue his own interest at the expense of the happiness of thousands, and if he is persuaded that any action will tend to his own interest, he is at liberty to do it, whatever may be the consequences to others.

Dr. Paley adopts the principle that all virtue consists in a regard to our own happiness, taking into view the whole of our existence. His definition is, however, a very complicated one, and deserves to be analysed.

Virtue," says he, "is the doing good to mankind, in obedience to the will of God, for the sake of everlasting happiness," according to which definition the good of mankind is the object, the will of God the rule, and everlasting happiness the motive of human virtue. If the question be asked, why we should seek the good of mankind, the answer is, from a regard to our everlasting happiness; and if the question be, why should we make the will of God the rule of our conduct, the answer must be the same; so that really all virtue is resolved into a regard to our own happiness.

Now every man desires to promote his own happiness, and according to Dr. Paley's theory, the only difference between an eminently good man and one of the opposite character is, that the one pursues a wiser course than the other; but they are both actuated by the same motives.

This theory loses sight of all intrinsic difference between moral good and evil, and admits the principle that happiness is the only conceivable good, and that anything is virtuous the tendency of which is to promote our greatest happiness.

A theory the opposite of that which makes a regard to private interest the ground of virtue, is the one which makes all virtue to consist in a regard to the public good. This is the theory of Bishop Cumberland in his work, De Legibus, and is not essentially different from the scheme of those who make all virtue to consist in disinterested benevolence. No doubt, much that deserves the name of virtue consists in good will to others, and in contributing to their welfare; but it is not correct to confine all virtuous actions to the exercise of benevolence. We can conceive of benevolence in a being who has no moral constitution. Something of this kind is observable in brute animals, and atheists may exercise benevolence to their friends. The indiscriminate exercise of benevolence to creatures, without any respect to their moral character, might appear to be an amiable attribute, but it could not properly be called a moral attribute. A prudent regard to our own welfare and happiness is undoubtedly a virtue. It has been considered so by the wisest of men, and we know that prudence was one of the four cardinal virtues of the heathen. As the whole is made up of parts, it is evident that if it is a virtue to promote the well-being of the whole, it must be so of each of the parts. The pursuit of our own happiness where it does not infringe on the rights of others, has nothing evil in it, but is approved by every impartial mind. Some who maintain that all virtue consists in benevolence, admit that we may seek our own happiness just as we seek that of our neighbour; but the human constitution is not formed to exercise that abstract impartiality. While we are bound to promote the welfare of our neighbour and of strangers, our obligation is still stronger to endeavour to secure our own happiness; and if a friend and a stranger stand in equal need of a benefit which we have it in our power to bestow, it is evidently our duty to consult first the welfare of our friend, other things being equal.

What Bishop Butler has said on this subject in his short treatise on "Virtue," is worthy of consideration: "It deserves

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