ELECTRICITY AND MAGNETISM.[1]

[Footnote 1: Introductory to the course of Lectures on Physics at

Washington University, St. Louis, Missouri--_Kansas City

Review._]

Prof. FRANCIS E. NIPHER.

It was known six hundred years before Christ that when amber is rubbed

it acquires the power of attracting light bodies. The Greek name for

amber, _elektron_, was afterward applied to the phenomenon. It was

also known to the ancients that a certain kind of iron ore, first

found at Magnesia, in Asia Minor, had the property of attracting

iron. This phenomenon was called magnetism. This is the history of

electricity and magnetism for two thousand years, during which these

facts stood alone, like isolated mountain peaks, with summits touched

and made visible by the morning sun, while the region surrounding and

connecting them lay hidden and unexplored.

In fact, it is only in more recent times that men could be found

possessing the necessary mental qualities to insure success in

physical investigation. Some of the ancients were acute observers, and

made valuable observations in descriptive natural history. They also

observed and described phenomena which they saw around them, although

often in vague and mystical terms.

They, however, were greatly lacking in power to discriminate

between the possible and the absurd, and so old wives' tales,

acute speculations, and truthful observations are strangely jumbled

together. With rare exceptions they did not contrive new conditions to

bring about phenomena which Nature did not spontaneously exhibit--they

did not experiment. They attempted to solve the universe in their

heads, and made little progress.

In mediæval times intellectual men were busy in trying to set each

other right, and in disputing and arguing with those who believed

themselves to be right. It was an era of intellectual pugilism,

and nothing was done in physics. In fact, this frame of mind is

incompatible with any marked success in scientific work.

The physical investigator cannot take up his work in the spirit of

controversy; for the phenomena and laws of Nature will not argue with

him. He must come as a learner, and the true man of science is content

to learn, is content to lay his results before his fellows, and is

willing to profit by their criticisms. In so far as he permits himself

to assume the mental attitude of one who defends a position, in so far

does he reveal a grave disqualification for the most useful scientific

work. Scientific truth needs no man's defense, but our individual

statements of what we believe to be truth frequently need criticism.

It is hardly necessary to remark, also, that critics are of various

degrees of excellence, and it seems that those in whom the habit of

criticism has become chronic are of comparatively little service to

the world.

The great harbinger of the new era was Galileo. There had been

prophets before him, and after him came a greater one--Newton. They

did nothing of note in electricity and magnetism, but they were filled

with the true spirit of science, they introduced proper and reasonable

methods of investigation, and by their great ability and distinguished

success they have produced a revolution in the intellectual world.

Other great men had also appeared, such as Leibnitz and Huyghens; and

it became very clear that the methods of investigation which had borne

such fruit in the days of Galileo were not disposed of completely

by his unwilling recantation; it became very clear that the new

civilization which was dawning upon Europe was not destined to the

rude fate which had overwhelmed the brilliant scientific achievements

of the Spanish Moors of a half century before.

Already in 1580, about the time when Galileo entered Pisa as a

student, Borroughs had determined the variation of the magnetic needle

at London, and we have upon the screen a view of his instrument, which

seems rude enough, in comparison with the elaborate apparatus of our

times. The first great work on electricity and magnetism was the "De

Magnete" of Gilbert, physician of Queen Elizabeth, published in

1600. Galileo, already famous in Europe, recognized in the methods of

investigation used by Gilbert the ones which he had found so fruitful,

and wrote of him, "I extremely praise, admire, and envy this author."

Gilbert made many interesting contributions to magnetism, which we

shall notice in another lecture, and he also found that sulphur,

glass, wax, and other bodies share with amber the property of being

electrified by friction. He concluded that many bodies could not be

thus electrified. Gray, however, found in 1729 that these bodies were

conductors of electricity, and his discoveries and experiments were

explained and described to the president of the Royal Society while on

his death bed, and only a few hours before his death. If precautions

are taken to properly insulate conductors, all bodies which differ

in any way, either in structure, in smoothness of surface, or even in

temperature, are apparently electrified by friction. In all cases

the friction also produces heat, and if the bodies rubbed are exactly

alike, heat only is produced.

An electrified body will attract all light bodies. This gutta percha

when rubbed with a cat's skin attracts these bits of paper, and this

pith ball, and this copper ball; it moves this long lath balanced on

its center, and deflects this vertical jet of water into a beautiful

curve.

If a conductor is to be electrified, it must be supported by bad

conductors. This brass cylinder standing on a glass column has become

electrified by friction with cat's-skin. My assistant will stand upon

this insulating stool, and by stroking his hand you will observe that

with his other hand he can attract this suspended rod of wood, and you

will hear a feeble spark when I apply my knuckle to his.

Du Fay, of Paris, discovered what he called two kinds of electricity.

He found that a glass rod rubbed with silk will repel another glass

rod similarly rubbed, but that the silk would attract a rubbed

glass rod. We express the facts in the well-known law that like

electricities repel each other, and unlike attract. For a long time

the nature of the distinctions between the two electricities was not

understood. It was found later that when the two bodies are rubbed

together they become oppositely electrified, and that the two

electricities are always generated in equal quantity; so that if the

two bodies are held in contact after the rubbing has ceased the

two electricities come together again and the electrical phenomena

disappear. They have been added together, and the result is zero.

Franklin proposed to call these electricities positive and negative.

These names are well chosen, but we do not know any reason why one

should be called positive rather than the other. The electricity

generated on glass when rubbed with silk is called positive.

Let us now examine the distinction between positive and negative

electricities somewhat more closely, aiding ourselves by two cases

which are somewhat analogous.

Two air-tight cylinders, A and B, contain air at ordinary pressure.

The cylinders are connected by a tube containing an air-pump in such a

way that, when the pump is worked, air is taken from A and forced into

B. To use the language of the electricians, we at once generate two

kinds of pressure. The vessels have acquired new properties. If we

open a cock in the side of either vessel, we hear a hissing sound, if

a light body is placed before the opening in A it would be attracted,

and before the opening in B it would be repelled. Now this is only

roughly analogous to the case of the electrified bodies, but the

analogy will nevertheless aid us in our study. If the two vessels are

first connected with the air, and then closed up and the pump is set

to work, we increase the pressure in B and diminish the pressure in

A. To do this requires the expenditure of a quantity of work. If the

cylinders are connected by an open tube--a conductor--the difference

in pressure disappears by reason of a flow of gas from one vessel to

the other.

If we had a pump by means of which we could pump heat from one body

into another, starting with two bodies at the same temperature, the

temperature of one body would increase and that of the other would

diminish. If we knew less than we do of heat, we might well discuss

whether the plus sign should be applied to the heat or to the cold,

because these names were coined by people who knew very little about

the subject except that these bodies produce different sensations when

they come in contact with the human body.

Furthermore, we find that whether the hand is applied to a very hot

body or to a very cold body, the physiological effect is the same. In

each case the tissue is destroyed and a burn is produced. Shall we now

say that this burn is produced by an unusual flow of heat from the hot

body to the hand, or from the hand to the cold body, or shall we say

that it is due to an unusual flow of cold from the cold body to the

hand, or from the hand to the hot body?

Logically these expressions are identical; still we have come to

prefer one of them. It is because we have learned that in those bodies

which our fathers called hot, the particles are vibrating with greater

energy than in cold bodies, that we prefer to say that heat is added

and not cold subtracted, when a cold body becomes less cold.

Now to come back to our electrified bodies. Let us suppose that this

gutta percha, and this cat's-skin are not electrified. That means that

their electrical condition is the same as that of surrounding bodies.

Let us also suppose that their thermal condition is the same as

surrounding bodies, ourselves included--that is, they are neither hot

nor cold. We express these conditions in other words by saying

that the bodies have the same electrical _potential_ and the same

temperature.

Temperature in heat is analogous to potential in electricity. As

soon as adjacent bodies are at different temperatures, we have

the phenomena which reveal to us the existence of heat. As soon as

adjacent bodies have different electrical potentials, we have the

phenomena which reveal the existence of electricity. As soon as

adjacent regions in the air are at different pressures, we have

phenomena which reveal the existence of air.

Bodies all tend to preserve the same temperature and also the same

electrical potential. Any disturbances in electrical equilibrium are

much more quickly obliterated than in case of thermal equilibrium,

and we therefore see less of electrical phenomena than of thermal. In

thunder storms we see such disturbances, and with delicate instruments

we find them going on continuously. Changes in temperature occurring

on a large scale in our atmosphere, occurring in these gas jets,

in our fires, in the axles of machinery, and in thousands of other

places, are so familiar that we have ceased to wonder at them.

If we rub these two bodies together, the potential of the two is no

longer the same. We do not know which one has become greater, and in

this respect our knowledge of electricity is less complete than of

heat. We assume that the gutta percha has become negative. If we now

leave these bodies in contact, the potential of the cat's skin will

diminish and that of the gutta percha will increase until they have

again reached a common potential--that of the earth. As in the case of

heat and cold, we may say either that this has come about by a flow of

positive electricity from the cat's skin to the gutta percha, or by

a flow of negative electricity in the opposite direction, for these

statements are identical.

In case of our gas cylinders, the gas tends to leak out of the vessel

where the pressure is great into the vessel where it is small. The

heat tends to leak out of a body of high temperature into the colder

one, or the cold tends to go in the opposite direction. Similarly, the

plus electricity tends to flow from the body having a high potential,

to the body having a low potential, or the minus electricity tends to

go in the opposite direction.

* * * * *

[ENGINEERING.]

Scientific American Supplement, No. 488, May 9, 1885 · 第 34 / 59 题