The apparatus was quickly perfected by coating both the inside and

outside of a jar with tin foil, applying the charge by means of a wire

or chain to the inside coating and allowing the outer one to stand

upon the earth or upon a conducting substance in electrical contact

with the latter. The exaltation of spirit with which the discovery was

hailed by the _savants_ appears to have been extraordinary--one

student who took a discharge through his body being reported to state

that he would not have missed the experience for a fabulous

consideration, and that he would not repeat it if it were to save his

life. In reality the advance was enormous; it gave a means for

literally bottling up electricity in quantities previously unthought

of. The prime conductor of an electrical machine could not retain any

considerable quantity of electricity for the reason that, a certain

small intensity of electrification having been reached, the addition

operated to upset the balance, so to speak, and the electricity

escaped by a sudden (disruptive) discharge, or spark, or by the brush

discharge already alluded to. With the Leyden jar, however, as fast as

electricity was supplied to the inside coating it became "bound" there

by the charge of opposite sign accumulating on the outside, and the

limit of capacity of the jar was simply one of strength of the glass:

if too much electricity was supplied, the stress of mutual attraction

between the two charges relieved itself by destroying the jar.

Although Professor Muschenbroeck discovered the principle in the

manner above referred to, it appears extremely probable that two other

investigators, working independently, also did the same. One Cuneus

and a monk named Kleist each claimed the honor of original invention

of the condenser.

About 1747 the first gun was fired by electricity; this was

accomplished by Sir William Watson, who also succeeded in kindling

alcohol and gas by means of a drop of cold water and even with ice.

The same experimenter reversed the ordinary procedure of causing the

electric influence to pass from an electrified body to the one to be

experimented upon, the latter being unelectrified, by electrifying the

latter, and then producing the desired effect by approaching it to an

unelectrified one.

A party of the Royal Society with Watson as chief operator instituted

a series of researches on a grand scale to determine, if possible, the

velocity of the electric discharge, and arrived at a number of

conclusions which, however, were of a decidedly negative nature. The

most important of these were as follows: That they could not observe

any interval between the instant of applying the discharge to one end

of the line and its reception at the other; that the destructive

effects of discharge are greater through bad conductors than through

good ones; that conduction is equally powerful whether occurring

through earth or water.

Just previous to this there had been some brilliant experiments

carried on in France, and the discharge had been conveyed through

twelve thousand feet of circuit, including the acre basin of the

Tuileries, but they had not been performed as systematically, or with

the definite objects in view, as had the English experiments.

The following year the Royal Society continued its researches on a

larger scale than previously, using 12,276 feet of wire, and found

that even through that length the velocity was practically

instantaneous.

Watson urged as a theory that electrical disturbances were caused by

influx or efflux of a single electric fluid from the state of normal

electrification, thus differing from Dufay in his opinion as to the

existence of two fluids. He was led to this belief by observing that

he obtained a larger spark between two oppositely electrified bodies

than from either to the earth.

From this time on there appears upon the scene a host of workers in

this field, one of the most prominent being the distinguished

American, Benjamin Franklin. Somewhat previous to his remarkable work,

or about 1750, Boze made certain discoveries in the matter of the

surface tension of conducting liquids being diminished by

electrification, and Mowbray and Nollet ascertained that the

vegetation of flowers and of vegetating seeds was hastened by

electrifying them.

Franklin (born 1706, died 1790) made the important discovery of the

active discharge of electricity from an electrified body by points as

well as the converse of it--i. e., that electricity was rapidly

abstracted from a charged atmosphere by points. This enabled him to

increase the efficiency of the electrical machine by adding a

comb-shaped series of points to the collector of the prime conductor.

Up to this time, although the identity of lightning with electricity

had long been suspected, it had not been at all established, and to

Franklin may be said to belong the honor of doing so, although in

this, as in the case of the invention of the Leyden jar, there appears

to have been successful contemporaneous research elsewhere. Before

performing his great experiment Franklin published a book strongly

supporting the belief in the identity of the two. Once having

conceived the idea of drawing electricity from the upper atmosphere,

he unfortunately lost some time through waiting for the completion of

the spire of a certain church in Philadelphia, from the top of which

he hoped to be able to collect electricity by means of a wire, but

finally hit upon the device which now fills much the same place in

connection with his memory that the classical cherry tree does with

Washington's--the lightning-collecting kite. This apparatus was very

simply constructed, and had a pointed wire projecting a short distance

above the framework. It was controlled, and electrical connection

made, by an ordinary string which terminated in a short length of silk

ribbon to protect the person from possible injury, and to give

electricity a chance to accumulate in the system, by insulating the

"line." At the end of the string proper Franklin fastened a metallic

key. In company with his son he flew the kite during a thunderstorm

which occurred in June, 1752; for some time no electric disturbance

approached the neighborhood, and he was on the point of abandoning the

experiment when he observed what he had been waiting for--the outer

fibers of the string standing out from the latter by repulsive

force--and, applying his knuckle to the key, he drew a spark.

Subsequently, when the rain soaked the string and caused it to conduct

much better, there was a fine supply of electricity, and Franklin

charged a Leyden jar from the key, thus achieving the actual storage

of "lightning."

He continued his investigations in atmospheric electricity, and

discovered that the electrification of the clouds (or of the upper

atmosphere) was sometimes positive and sometimes negative. The

invention of the lightning rod is due to him.

Franklin sided with Watson in his belief in the single nature of the

electric fluid.

As intimated above, atmospheric electricity appears to have been

collected independently about the same time in Europe, and certain

very daring and dangerous experiments were performed there. One sad

occurrence, as a result, was the death of Professor Richman, in St.

Petersburg, in 1753. Richman, in company with a friend, Sokolow, was

taking observations on an electroscope connected with an iron rod

which terminated in the apartment and extended in the other direction

above the roof of the building. During the progress of their

experiments a violent peal of thunder was heard in the neighborhood,

and Richman bent to examine the instrument. In doing so he approached

his head to within a foot of the end of the rod, and Sokolow saw a

ball of fire "about the size of a man's fist" shoot from it to

Richman's head with a terrific report. The stroke was, of course,

immediately fatal, and what we now know as the return shock stupefied

and benumbed Sokolow. The unfortunate event served as a warning to

other daring experimenters.

Canton, another prominent worker in this field, discovered that the

so-called vitreous electricity was not necessarily always developed by

the friction of glass, as had hitherto been believed to be invariably

the case. By applying different rubbers to glass he obtained either

positive or negative at pleasure. This at once disposed of the idea

that one kind of electricity resided in certain bodies and its

opposite in others. Canton also made the interesting discovery that

glass, amber, rock crystal, etc., when taken out of mercury, were all

electrified positively. He was thus enabled to make the improvement in

the electrical machine of coating its rubber with an amalgam rich in

mercury, which greatly enhanced its powers.

Among the numerous names now coming into prominence must be mentioned

those of Beccaria, Symmer, Delaval, Wilson, Kinnersley, Wilcke, and

Priestley.

The first named, Father Beccaria, was a celebrated Italian physicist

who did most valuable work in connection with atmospheric electricity,

and who published several classical works on that and allied subjects.

Among these may be mentioned his _Lettre del Elettricità_, 1758, and

_Experimenta_, 1772. He ascertained that water is not by any means a

good conductor, as it had previously been supposed to be, and, by

using pure water, he caused the electric spark to become visible in

it, a phenomenon capable of occurring only through media almost

nonconducting. In these experiments he used thick glass tubes with

wires led through the opposite ends, the latter being sealed, and the

tubes filled with water. These were invariably shattered by the

passage of the spark on account of the accompanying elevation of

temperature, which caused expansion. He also established the facts

that the atmosphere adjacent to an electrified body acquires

electrification of the same sign by abstracting electricity from the

body, and that the air then parts with its electricity very slowly. He

advanced the theory that there is a mutual repulsion between the

particles of the electric fluid and those of air, and that a temporary

vacuum is formed at the moment of the passage of a disruptive

discharge or spark.

Robert Symmer, in 1759, described some most entertaining experiments,

making use of the opposite electrifications of superposed stockings of

different materials or merely of different colors (the dye matters in

the latter case causing differentiation). If, in a dry atmosphere, a

silk stocking be drawn over the leg and a woolen one pulled over it,

the two will be found, upon being removed, to be very powerfully

electrified in opposite senses. If the four stockings of two such

pairs be used and then suspended together, they will indulge in

remarkable antics due to each of the silk stockings trying to attract

both of the woolen ones, and _vice versa_, and, on the other hand,

each of each kind repelling the other. The amount of electrical

attraction and repulsion produced in this simple way in a dry

atmosphere is remarkable. The experiment may also be performed with

all silk stockings, one pair white and the other black.

Symmer advanced the theory of two fluids coexisting in all matter (not

independently of each other, as had been previously supposed), which

by mutual counteractions produced all electrical phenomena. His

conception was that a body, positively electrified, did not exist in

that condition because of the possession of a charge of a positive (as

distinct from a negative) electric fluid which it had not held before,

and did not hold in a normal state; nor that it possessed a greater

share of a single electric fluid than it did in an unelectrified

condition, as had been believed by Franklin and Watson, and by Dufay

respectively; but that such a body contained both positive

and negative electricities which, when the body behaved as

"unelectrified," entirely counteracted each other, but which, on the

other hand, caused a positive or negative charge to be evinced should

either positive or negative electricity respectively preponderate.

Æpinus was the author of another notable theory, of which we must omit

further mention for want of space.

Disjointed observations connected with animal electricity had been

accumulating for many centuries. The first chronicled note that refers

to the subject dates back to 676 A. D. Whether or not entirely by

chance, the Arabians named the electric eel, or torpedo, in a way that

impresses us now as singularly felicitous, _raad_ (the lightning).

Toward the end of the last century Redi discovered that the shock was

sometimes conveyed through the line and rod to the fisherman, and

Kampfer compared the effects to those of electrical discharges. It

does not appear, however, that the resemblance was actually believed

to be more than accidental until Bancroft urged, in the last ten years

of the eighteenth century, the view which was shortly proved.

Investigation since has shown that several other aquatic animals

possess this astonishing manifestation of vitality, notably the

_Gymnotus electricus_ (Surinam eel), the _Trichiurus electricus_, and

the _Tetraodon electricus_. Humboldt gives an account of wonderful

battles in South America between gymnoti and wild horses. In fact, the

most expeditious method, if not the most humane one, of capturing

these alarming creatures appears to be to drive horses into the pond

inhabited by them, and to allow the eels to exhaust their strength by

repeated electric discharges before endeavoring to bring them to land

by other means.

Cavendish was one of the most noted experimental investigators in the

electrical field during the latter third of the eighteenth century.

His work was remarkably accurate, considering the lack of a proper

equipment for taking observations incident to operations in those

days. He computed the relative conductivities of iron and water as

four hundred million to unity, and found that the addition of but one

part of common salt to one hundred of water increased the conductivity

of the latter a hundredfold. A twenty-six-per-cent solution of salt he

found to possess only seven and one quarter times the conductivity of

the extremely weak one mentioned. He also established the law that the

capacity of condensers (of which the previously mentioned Leyden jar

is an example) varies directly as the active area, and inversely as

the distance separating the conducting surfaces. It was reserved for

later investigators to make the grand discoveries which relate to

electrochemical dissociation, but Cavendish succeeded in accurately

determining the ratio of combination of the elements of water in a

method which superficially suggests the inverse of electrolytic

decomposition--i. e., by inducing the combination of hydrogen and

oxygen by the electric spark in the instrument known as the

eudiometer.

Hard on the heels of this work came news of Galvani's remarkable

discovery (1790) of the fact that freshly amputated frogs' legs, on

being touched along the lines of the muscles by dissimilar metals,

were powerfully agitated. We can only speak of this discovery as the

stumbling on to an isolated fact, for it was reserved for Volta to

establish the generalization that a current is produced in the

conductor joining dissimilar metals when the latter are both in

contact with a suitable electrolyte (or liquid capable both of

conducting electricity and of acting on one, and incidentally also

sometimes both, of the metals). Meantime (Du Bois-Reymond observes),

"wherever frogs were to be found, and where two different kinds of

metal could be procured, everybody was anxious to see the mangled

limbs of frogs brought to life in this wonderful way. Physiologists

believed that at last they should realize their visions of a vital

power, and physicians that no cure was impossible."

Volta first discovered merely the fact of electrification by contact.

He wrote to Galvani: "I don't need your frog. Give me two metals and a

moist rag, and I will produce your animal electricity. Your frog is

nothing but a moist conductor, and in this respect it is inferior to

my wet rag!" Nobili, nevertheless, in 1825 proved the existence of

galvanic currents in muscles.

Later on Volta invented the "_couronne des tasses_" (crown of cups),

thus at the same time adopting the general form of cell used, with

modifications, to-day, and producing the higher electromotive force,

or electrical pressure, consequent on the multiplication of the cells

in a series battery.

Just before Volta's celebrated communication to the Royal Society, in

1800, Fabroni, of Florence, in discussing Galvani's phenomenon, went

to the root of the matter by suggesting that the energy of chemical

action was at the bottom of galvanic manifestations, and he was warmly

upheld in this contention by Sir Humphry Davy, who, upon the

publication of Volta's discoveries, constructed a most elaborate

battery with which (apparently about 1806) he produced the arc light

between carbon pencils.

In the year referred to, Davy published the results of a series of

experiments of enormous significance, among other things of the

isolation of the alkali metals, sodium and potassium, whose existence

had hitherto not been dreamed of. The simple electrolytic

decomposition of water had been accomplished by Nicolson and Carlisle

in the last year of the eighteenth century. Sir W. S. Harris says: "A

series of new substances was speedily discovered, the existence of

which had never before been imagined. Oxygen, chlorine, and acids were

all dragged, as it were, to the positive pole, while metals,

inflammable bodies, alkalies, and earths became determined to the

negative pole of the battery. When wires connected with each extremity

of the new battery were tipped with prepared and well-pointed

charcoal, and the points brought near each other, then a most intense

and pure evolution of light followed, which on separating the points

extended to a gorgeous arc." It was at first supposed that the

galvanic or voltaic electricity was distinct from the so-called

"frictional" or "ordinary" electricity.

A distinguished contemporary of Cavendish was Coulomb, the value of

whose work in developing certain exceedingly important mathematical

laws with regard to action at a distance, surface densities, and rates

of charge dissipation can hardly be overestimated. His name was given

to the torsion balance which, since his day, has been the standard

instrument for measuring electric and magnetic attractions and

repulsions. The importance of his work has since been recognized by

the perpetuation of his name in connection with the unit of quantity

of electricity, as that of Volta has been honored by its use,

abbreviated (volt), to designate the unit of electrical tension or

pressure.

Certain highly instructive and interesting data were accumulated about

this time by Volta, Laplace, Saussure, and the renowned chemist

Lavoisier, in connection with the subject of electrification produced

when evaporation, and the liberation of gases and vapors in general

from any cause, occurs. The liquid, solid, or mixture liberating the

gas was contained in a metallic dish and the resultant electrification

of the latter examined qualitatively. Volta's observations led him to

conclude that the electrification was always negative, but Saussure

demonstrated finally that its sign was dependent on the material of

the dish. These experimenters covered, between them all, a somewhat

extensive field, examining, among other things, the electrification

resulting from the ebullition of various liquids, from the ordinary

combustion of fuel, and from the decomposition of acids by metals to

liberate hydrogen.

About the end of the first decade of the century Poisson attacked the

phenomena of electricity analytically, and succeeded in demonstrating

the right of electrical investigation to rank among the exact

sciences. Of his most important mathematical propositions is one in

which, assuming as a working hypothesis the existence of two mutually

attracting fluids, he deduced formulæ covering the distribution of

these fluids on the surfaces of two conducting spheres, in or out of

contact.

A great deal of work was done during the end of the last century and

the beginning of the present one on what is now known as

pyro-electrification. The Abbé Haüy discovered that fragments of

tourmaline crystal exhibited opposite electrifications on opposite

extremities of their lines of cleavage. It is this crystal also which

has unusually remarkable powers of polarizing light, and which, under

electro-magnetic stress, suffers modifications of the latter

property. Haüy investigated the field with much diligence, and

succeeded in cataloguing a large number of natural crystals by the

side of tourmaline. The subject was amplified later by Sir David

Brewster, who added a series of artificial crystalline salts to the

list of pyro-electrical materials, among them, notably, hydro-potassic

(and sodic) tartrate. The property was found not always to reside on

these substances, but to be developed by heating them. Brewster found

that even powdered tourmaline exhibited opposite electrifications on

the opposite extremities of each tiny particle, causing the latter to

act, so far as attractions and repulsions went, as infinitesimal

magnets.

Our rapid and imperfect survey has now brought us to the threshold of

the great activity in electrical work elicited by the tremendous

discovery, made by Professor Oersted, of Copenhagen, of the existence

of the electro-magnetic field. It happens that two of the most amiable

and estimable individuals that have ever devoted their lives to

scientific research stand out in this connection head and shoulders

above all other investigators--Ampère and Faraday, the latter sixteen

years younger than the former and destined to long survive him.

WINGLESS BIRDS.

BY PHILIPPE GLANGEAUD.

It is often said that there are no rules without exceptions. We

purpose to test the truth of this maxim once more. Fishes are made to

live in water, but some of them pass the greater part of their

existence in mud. Some even perch upon trees, thus competing with

birds, whose kingdom is the air, and which are able, with the aid of

their wings, to plunge into space and travel rapidly over considerable

distances. Yet there are birds, deprived by Nature, which do not

possess the wing characteristic of the feathered tribe, and are

consequently, like the majority of animals, pinned to the soil.

Birds do not all have equal power of flight, which is closely related

to the extent of the development of their wings. There exist all

grades in the spread of wings between that of the condor, which is

four times the length of the body, whereby the bird is able to rise to

the height of nearly twenty-five thousand feet, and the little

winglets of the auk, which are of no use to it. The penguins have

still smaller wings, which are nothing more than short, flattened

stumps, without proper feathers and covered with a fine, hairlike down

which might be taken for scales.

Another group of birds exists, called appropriately _Brevipennes_,

the wings of which are so poorly developed as to be wholly unsuitable

for flight. As an offset and just compensation for this, their long

and robust legs permit them to run with extraordinary speed. For that

reason they have been called running birds, in distinction from other

kinds that constitute the group of flying birds. Among them are some

gigantic birds, and also some that have no visible wings on the

outside of their bodies, and may therefore be properly called

wingless.

The ostrich is a member of this group. With its bare, callous head and

short bill, its long, featherless neck, and its massive body,

supported by long, half-bare legs, ending in two large toes; its very

short wings, formed of soft and flexible feathers; and its

plume-shaped tail, it presents a very special appearance among the

birds.

The nandous, the American representatives of the ostrich, have still

shorter wings, which have no _remigia_ at all, and terminate in a

horny appendage, and they have no tail feathers.

Appletons' Popular Science Monthly, December 1899 Vol. LVI, November, 1899 to April, 1900 · 第 10 / 16 段