SIR,

§ 1. There will be the same explosion and shock if the electrified

phial is held in one hand by the hook, and the coating touched with

the other, as when held by the coating, and touched at the hook.

2. To take the charged phial safely by the hook, and not at the same

time diminish its force, it must first be set down on an electric

_per se_.

3. The phial will be electrified as strongly, if held by the hook,

and the coating applied to the globe or tube; as when held by the

coating, and the hook applied[33].

4. But the _direction_ of the electrical fire being different in the

charging, will also be different in the explosion. The bottle charged

through the hook, will be discharged through the hook; the bottle

charged through the coating, will be discharged through the coating,

and not otherways; for the fire must come out the same way it went in.

5. To prove this, take two bottles that were equally charged through

the hooks, one in each hand: bring their hooks near each other, and

no spark or shock will follow; because each hook is disposed to

give fire, and neither to receive it. Set one of the bottles down

on glass, take it up by the hook, and apply its coating to the hook

of the other; then there will be an explosion and shock, and both

bottles will be discharged.

6. Vary the experiment, by charging two phials equally, one through

the hook, the other through the coating: hold that by the coating

which was charged through the hook; and that by the hook which was

charged through the coating: apply the hook of the first to the

coating of the other, and there will be no shock or spark. Set that

down on glass which you held by the hook, take it up by the coating,

and bring the two hooks together: a spark and shock will follow, and

both phials be discharged.

In this experiment the bottles are totally discharged, or the

equilibrium within them restored. The _abounding_ of fire in one of

the hooks (or rather in the internal surface of one bottle) being

exactly equal to the _wanting_ of the other: and therefore, as each

bottle has in itself the _abounding_ as well as the _wanting_,

the wanting and abounding must be equal in each bottle. See § 8,

9, 10, 11. But if a man holds in his hands two bottles, one fully

electrified, the other not at all, and brings their hooks together,

he has but half a shock, and the bottles will both remain half

electrified, the one being half discharged, and the other half

charged.

7. Place two phials equally charged on a table at five or six inches

distance. Let a cork-ball, suspended by a silk thread, hang between

them. If the phials were both charged through their hooks, the

cork, when it has been attracted and repelled by the one, will not

be attracted, but equally repelled by the other. But if the phials

were charged, the one through the hook, and the other[34] through

the coating, the ball, when it is repelled from one hook, will be as

strongly attracted by the other, and play vigorously between them,

fetching the electric fluid from the one, and delivering it to the

other, till both phials are nearly discharged.

8. When we use the terms of _charging_ and _discharging_ the phial,

it is in compliance with custom, and for want of others more

suitable. Since we are of opinion that there is really no more

electrical fire in the phial after what is called its _charging_,

than before, nor less after its _discharging_; excepting only the

small spark that might be given to, and taken from the non-electric

matter, if separated from the bottle, which spark may not be equal to

a five hundredth part of what is called the explosion.

For if, on the explosion, the electrical fire came out of the bottle

by one part, and did not enter in again by another, then, if a man,

standing on wax, and holding the bottle in one hand, takes the spark

by touching the wire hook with the other, the bottle being thereby

_discharged_, the man would be _charged_; or whatever fire was lost

by one, would be found in the other, since there was no way for its

escape: but the contrary is true.

9. Besides, the phial will not suffer what is called a _charging_,

unless as much fire can go out of it one way, as is thrown in by

another. A phial cannot be charged standing on wax or glass, or

hanging on the prime conductor, unless a communication be formed

between its coating and the floor.

10. But suspend two or more phials on the prime conductor, one

hanging on the tail of the other; and a wire from the last to the

floor, an equal number of turns of the wheel shall charge them all

equally, and every one as much as one alone would have been. What is

driven out at the tail of the first, serving to charge the second;

what is driven out of the second charging the third; and so on. By

this means a great number of bottles might be charged with the same

labour, and equally high, with one alone; were it not that every

bottle receives new fire, and loses its old with some reluctance, or

rather gives some small resistance to the charging, which in a number

of bottles becomes more equal to the charging power, and so repels

the fire back again on the globe, sooner in proportion than a single

bottle would do.

11. When a bottle is charged in the common way, its _inside_ and

_outside_ surfaces stand ready, the one to give fire by the hook,

the other to receive it by the coating; the one is full, and ready

to throw out, the other empty and extremely hungry; yet as the

first will not _give out_, unless the other can at the same instant

_receive in_; so neither will the latter receive in, unless the first

can at the same instant give out. When both can be done at once, it

is done with inconceivable quickness and violence.

12. So a straight spring (though the comparison does not agree in

every particular) when forcibly bent, must, to restore itself,

contract that side which in the bending was extended, and extend that

which was contracted; if either of these two operations be hindered,

the other cannot be done. But the spring is not said to be _charged_

with elasticity when bent, and discharged when unbent; its quantity

of elasticity is always the same.

13. Glass, in like manner, has, within its substance, always the

same quantity of electrical fire, and that a very great quantity in

proportion to the mass of glass, as shall be shewn hereafter.

14. This quantity, proportioned to the glass, it strongly and

obstinately retains, and will have neither more nor less, though it

will suffer a change to be made in its parts and situation; _i. e._

we may take away part of it from one of the sides, provided we throw

an equal quantity into the other.

15. Yet when the situation of the electrical fire is thus altered in

the glass; when some has been taken from one side, and some added to

the other, it will not be at rest or in its natural state, till it

is restored to its original equality. And this restitution cannot

be made through the substance of the glass, but must be done by a

non-electric communication formed without, from surface to surface.

16. Thus, the whole force of the bottle, and power of giving a

shock, is in the GLASS ITSELF; the non-electrics in contact with the

two surfaces, serving only to _give_ and _receive_ to and from the

several parts of the glass; that is, to give on one side, and take

away from the other.

17. This was discovered here in the following manner: Purposing to

analyse the electrified bottle, in order to find wherein its strength

lay, we placed it on glass, and drew out the cork and wire which

for that purpose had been loosely put in. Then taking the bottle

in one hand, and bringing a finger of the other near its mouth, a

strong spark came from the water, and the shock was as violent as

if the wire had remained in it, which shewed that the force did not

lie in the wire. Then to find if it resided in the water, being

crowded into and condensed in it, as confined by the glass, which

had been our former opinion, we electrified the bottle again, and

placing it on glass, drew out the wire and cork as before; then

taking up the bottle, we decanted all its water into an empty bottle,

which likewise stood on glass; and taking up that other bottle, we

expected, if the force resided in the water, to find a shock from

it; but there was none. We judged then that it must either be lost

in decanting, or remain in the first bottle. The latter we found to

be true; for that bottle on trial gave the shock, though filled up

as it stood with fresh unelectrified water from a tea-pot.--To find,

then, whether glass had this property merely as glass, or whether

the form contributed any thing to it; we took a pane of sash-glass,

and laying it on the hand, placed a plate of lead on its upper

surface; then electrified that plate, and bringing a finger to it,

there was a spark and shock. We then took two plates of lead of equal

dimensions, but less than the glass by two inches every way, and

electrified the glass between them, by electrifying the uppermost

lead; then separated the glass from the lead, in doing which, what

little fire might be in the lead was taken out, and the glass being

touched in the electrified parts with a finger, afforded only very

small pricking sparks, but a great number of them might be taken from

different places. Then dextrously placing it again between the leaden

plates, and compleating a circle between the two surfaces, a violent

shock ensued.--Which demonstrated the power to reside in glass as

glass, and that the non-electrics in contact served only, like the

armature of a loadstone, to unite the force of the several parts, and

bring them at once to any point desired: it being the property of a

non-electric, that the whole body instantly receives or gives what

electrical fire is given to or taken from any one of its parts.

18. Upon this we made what we called an _electrical-battery_,

consisting of eleven panes of large sash-glass, armed with thin

leaden plates, pasted on each side, placed vertically, and supported

at two inches distance on silk cords, with thick hooks of leaden

wire, one from each side, standing upright, distant from each other,

and convenient communications of wire and chain, from the giving

side of one pane, to the receiving side of the other; that so the

whole might be charged together, and with the same labour as one

single pane; and another contrivance to bring the giving sides,

after charging, in contact with one long wire, and the receivers

with another, which two long wires would give the force of all the

plates of glass at once through the body of any animal forming the

circle with them. The plates may also be discharged separately, or

any number together that is required. But this machine is not much

used, as not perfectly answering our intention with regard to the

ease of charging, for the reason given, _Sec. 10._ We made also of

large glass panes, magical pictures, and self-moving animated wheels,

presently to be described.

19. I perceive by the ingenious Mr. Watson's last book, lately

received, that Dr. Bevis had used, before we had, panes of glass to

give a shock[35]; though, till that book came to hand, I thought to

have communicated it to you as a novelty. The excuse for mentioning

it here is, that we tried the experiment differently, drew different

consequences from it (for Mr. Watson still seems to think the fire

_accumulated on the non-electric_ that is in contact with the glass,

p. 72) and, as far as we hitherto know, have carried it farther.

20. The magical picture[36] is made thus. Having a large metzotinto

with a frame and glass, suppose of the KING (God preserve him) take

out the print, and cut a pannel out of it near two inches distant

from the frame all round. If the cut is through the picture it is not

the worse. With thin paste, or gum-water, fix the border that is cut

off on the inside the glass, pressing it smooth and close; then fill

up the vacancy by gilding the glass well with leaf-gold, or brass.

Gild likewise the inner edge of the back of the frame all round,

except the top part, and form a communication between that gilding

and the gilding behind the glass: then put in the board, and that

side is finished. Turn up the glass, and gild the fore side exactly

over the back gilding, and when it is dry, cover it, by pasting on

the pannel of the picture that hath been cut out, observing to bring

the correspondent parts of the border and picture together, by which

the picture will appear of a piece, as at first, only part is behind

the glass, and part before. Hold the picture horizontally by the

top, and place a little moveable gilt crown on the king's head. If

now the picture be moderately electrified, and another person take

hold of the frame with one hand, so that his fingers touch its inside

gilding, and with the other hand endeavour to take off the crown, he

will receive a terrible blow, and fail in the attempt. If the picture

were highly charged, the consequence might perhaps be as fatal[37] as

that of high treason, for when the spark is taken through a quire of

paper laid on the picture by means of a wire communication, it makes

a fair hole through every sheet, that is, through forty-eight leaves,

though a quire of paper is thought good armour against the push of

a sword, or even against a pistol bullet, and the crack is exceeding

loud. The operator, who holds the picture by the upper end, where

the inside of the frame is not gilt, to prevent its falling, feels

nothing of the shock, and may touch the face of the picture without

danger, which he pretends is a test of his loyalty.--If a ring of

persons take the shock among them, the experiment is called, _The

Conspirators_.

21. On the principle, in _Sec. 7_, that hooks of bottles, differently

charged, will attract and repel differently, is made an electrical

wheel, that turns with considerable strength. A small upright shaft

of wood passes at right angles through a thin round board, of about

twelve inches diameter, and turns on a sharp point of iron, fixed

in the lower end, while a strong wire in the upper end, passing

through a small hole in a thin brass plate, keeps the shaft truly

vertical. About thirty _radii_ of equal length, made of sash-glass,

cut in narrow strips, issue horizontally from the circumference of

the board, the ends most distant from the centre, being about four

inches apart. On the end of every one, a brass thimble is fixed. If

now the wire of a bottle electrified in the common way, be brought

near the circumference of this wheel, it will attract the nearest

thimble, and so put the wheel in motion; that thimble, in passing

by, receives a spark and thereby being electrified is repelled, and

so driven forwards; while a second being attracted, approaches the

wire, receives a spark, and is driven after the first, and so on till

the wheel has gone once round, when the thimbles before electrified

approaching the wire, instead of being attracted as they were at

first, are repelled, and the motion presently ceases.--But if

another bottle, which had been charged through the coating, be placed

near the same wheel, its wire will attract the thimble repelled by

the first, and thereby double the force that carries the wheel round;

and not only taking out the fire that had been communicated to the

thimbles by the first bottle, but even robbing them of their natural

quantity, instead of being repelled when they come again towards the

first bottle, they are more strongly attracted, so that the wheel

mends its pace, till it goes with great rapidity twelve or fifteen

rounds in a minute, and with such strength, as that the weight of one

hundred Spanish dollars with which we once loaded it, did not seem in

the least to retard its motion.--This is called an electrical jack;

and if a large fowl were spitted on the upright shaft, it would be

carried round before a fire with a motion fit for roasting.

22. But this wheel, like those driven by wind, water, or weights,

moves by a foreign force, to wit, that of the bottles. The

self-moving wheel, though constructed on the same principles, appears

more surprising. It is made of a thin round plate of window-glass,

seventeen inches diameter, well gilt on both sides, all but two

inches next the edge. Two small hemispheres of wood are then fixed

with cement to the middle of the upper and under sides, centrally

opposite, and in each of them a thick strong wire eight or ten

inches long, which together make the axis of the wheel. It turns

horizontally on a point at the lower end of its axis, which rests on

a bit of brass cemented within a glass salt-cellar. The upper end

of its axis passes through a hole in a thin brass plate cemented to

a long strong piece of glass, which keeps it six or eight inches

distant from any non-electric, and has a small ball of wax or metal

on its top, to keep in the fire. In a circle on the table which

supports the wheel, are fixed twelve small pillars of glass, at

about four inches distance, with a thimble on the top of each. On

the edge of the wheel is a small leaden bullet, communicating by

a wire with the gilding of the _upper_ surface of the wheel; and

about six inches from it is another bullet, communicating in like

manner with the _under_ surface. When the wheel is to be charged

by the upper surface, a communication must be made from the under

surface to the table. When it is well charged it begins to move; the

bullet nearest to a pillar moves towards the thimble on that pillar,

and passing by electrifies it, and then pushes itself from it; the

succeeding bullet, which communicates with the other surface of the

glass, more strongly attracts that thimble, on account of its being

before electrified by the other bullet; and thus the wheel encreases

its motion till it comes to such a height as that the resistance of

the air regulates it. It will go half an hour, and make one minute

with another twenty turns in a minute, which is six hundred turns

in the whole; the bullet of the upper surface giving in each turn

twelve sparks to the thimbles, which makes seven thousand two hundred

sparks: and the bullet of the under surface receiving as many from

the thimbles; those bullets moving in the time near two thousand five

hundred feet.--The thimbles are well fixed, and in so exact a circle,

that the bullets may pass within a very small distance of each of

them.--If instead of two bullets you put eight, four communicating

with the upper surface, and four with the under surface, placed

alternately, which eight, at about six inches distance, completes the

circumference, the force and swiftness will be greatly increased, the

wheel making fifty turns in a minute; but then it will not continue

moving so long.--These wheels may be applied, perhaps, to the ringing

of chimes,[38] and moving of light-made orreries.

23. A small wire bent circularly, with a loop at each end; let one

end rest against the under surface of the wheel, and bring the other

end near the upper surface, it will give a terrible crack, and the

force will be discharged.

24. Every spark in that manner drawn from the surface of the wheel,

makes a round hole in the gilding, tearing off a part of it in coming

out; which shews that the fire is not accumulated on the gilding, but

is in the glass itself.

25. The gilding being varnished over with turpentine varnish, the

varnish, though dry and hard, is burnt by the spark drawn through

it, and gives a strong smell and visible smoke. And when the spark

is drawn thro' paper, all round the hole made by it, the paper will

be blacked by the smoke, which sometimes penetrates several of the

leaves. Part of the gilding torn off is also found forcibly driven

into the hole made in the paper by the stroke.

26. It is amazing to observe in how small a portion of glass a

great electrical force may lie. A thin glass bubble, about an inch

diameter, weighing only six grains, being half filled with water,

partly gilt on the outside, and furnished with a wire hook, gives,

when electrified, as great a shock as a man can well bear. As the

glass is thickest near the orifice, I suppose the lower half, which

being gilt was electrified and gave the shock, did not exceed two

grains; for it appeared, when broken, much thinner than the upper

half.--If one of these thin bottles be electrified by the coating,

and the spark taken out through the gilding, it will break the glass

inwards, at the same time that it breaks the gilding outwards.

27. And allowing (for the reasons before given, § 8, 9, 10,) that

there is no more electrical fire in a bottle after charging, than

before, how great must be the quantity in this small portion of

glass! It seems as if it were of its very substance and essence.

Perhaps if that due quantity of electrical fire so obstinately

retained by glass, could be separated from it, it would no longer

be glass; it might lose its transparency, or its brittleness, or

its elasticity.--Experiments may possibly be invented hereafter, to

discover this.

27. We were surprised at the account given in Mr. Watson's book, of a

shock communicated through a great space of dry ground, and suspect

there must be some metalline quality in the gravel of that ground;

having found that simple dry earth, rammed in a glass tube, open at

both ends, and a wire hook inserted in the earth at each end, the

earth and wires making part of a circuit, would not conduct the least

perceptible shock, and indeed when one wire was electrified the other

hardly shewed any signs of its being in connection with it[39]. Even

a thoroughly wet packthread sometimes fails of conducting a shock,

though it otherwise conducts electricity very well. A dry cake of

ice, or an icicle held between two in a circle, likewise prevents the

shock, which one would not expect, as water conducts it so perfectly

well.--Gilding on a new book, though at first it conducts the shock

extremely well, yet fails after ten or a dozen experiments, though it

appears otherwise in all respects the same, which we cannot account

for[40].

28. There is one experiment more which surprises us, and is not

hitherto satisfactorily accounted for; it is this: Place an iron

shot on a glass stand, and let a ball of damp cork, suspended by a

silk thread, hang in contact with the shot. Take a bottle in each

hand, one that is electrified through the hook, the other through

the coating: Apply the giving wire to the shot, which will electrify

it _positively_, and the cork shall be repelled: then apply the

requiring wire, which will take out the spark given by the other;

when the cork will return to the shot: Apply the same again, and take

out another spark, so will the shot be electrified _negatively_,

and the cork in that case shall be repelled equally as before. Then

apply the giving wire to the shot, and give the spark it wanted, so

will the cork return: Give it another, which will be an addition to

its natural quantity, so will the cork be repelled again: And so

may the experiment be repeated as long as there is any charge in

the bottles. Which shews that bodies, having less than the common

quantity of electricity, repel each other, as well as those that have

more.

Chagrined a little that we have been hitherto able to produce nothing

in this way of use to mankind; and the hot weather coming on, when

electrical experiments are not so agreeable, it is proposed to put

an end to them for this season, somewhat humorously, in a party of

pleasure, on the banks of _Skuylkil_[41]. Spirits, at the same time,

are to be fired by a spark sent from side to side through the river,

without any other conductor than the water; an experiment which we

some time since performed, to the amazement of many[42].

A turkey is to be killed for our dinner by the _electrical shock_,

and roasted by the _electrical jack_, before a fire kindled by

the _electrified bottle_: when the healths of all the famous

electricians in England, Holland, France, and Germany are to be drank

in _electrified bumpers_[43], under the discharge of guns from the

_electrical battery_.

The Complete Works in Philosophy, Politics and Morals of the late Dr. Benjamin Franklin, Vol. 1 [of 3] · 第 95 / 291 题