SECTION XXX.

Discovery of Electro-magnetism—Deflection of the Magnetic Needle by a

Current of Electricity—Direction of the Force—Rotatory Motion by

Electricity—Rotation of a Wire and a Magnet—Rotation of a Magnet about

its Axis—Of Mercury and Water—Electro-Magnetic Cylinder or

Helix—Suspension of a Needle in a Helix—Electro-Magnetic

Induction—Temporary Magnets—The Galvanometer.

THE disturbing effects of the aurora and lightning on the mariner’s

compass had been long known. In the year 1819 M. Oersted, Professor of

Natural Philosophy at Copenhagen, discovered that a current of Voltaic

electricity exerts a powerful influence on a magnetized needle. This

observation has given rise to the theory of electro-magnetism—one of the

most interesting sciences of modern times, whether it be considered as

leading us a step farther in generalization, by identifying two agencies

hitherto referred to different causes, or as developing a new force,

unparalleled in the system of the world, which, overcoming the

retardation from friction, and the obstacle of a resisting medium,

maintains a perpetual motion as long as the action of a Voltaic battery

is continued.

When the two poles of a Voltaic battery are connected by a metallic

wire, so as to complete a circuit, the electricity flows without

ceasing. If a straight portion of that wire be placed parallel to, and

horizontally above, a magnetized needle at rest in the magnetic

meridian, but freely poised like the mariner’s compass, the action of

the electric current flowing through the wire will instantly cause the

needle to change its position. Its extremity will deviate from the north

towards the east or west, according to the direction in which the

current is flowing; and, on reversing the direction of the current, the

motion of the needle will be reversed also. The numerous experiments

that have been made on magnetism and electricity, as well as those on

the various relative motions of a magnetic needle under the influence of

galvanic electricity, arising from all possible positions of the

conducting wire, and every direction of the Voltaic current, together

with all the other phenomena of electro-magnetism, are explained by Dr.

Roget in some excellent articles on these subjects in the Library of

Useful Knowledge.

All experiments tend to prove that the force emanating from the electric

current, which produces such effects on the magnetic needle, acts at

right angles to the current. The action of an electrical current upon

either pole of a magnet has no tendency to cause the pole to approach or

recede, but to rotate about it. If the stream of electricity be supposed

to pass through the centre of a circle whose plane is perpendicular to

the current, the direction of the force exerted by the electricity will

always be in the tangent to the circle, or at right angles to its radius

(N. 223). Consequently, the tangential force of the electricity has a

tendency to make the pole of a magnet move in a circle round the wire of

the battery.

Rotatory motion was suggested by Dr. Wollaston. Dr. Faraday was the

first who actually succeeded in making the pole of a magnet rotate about

a vertical conducting wire. In order to limit the action of the

electricity to one pole, about two-thirds of a small magnet were

immersed in mercury, the lower end being fastened by a thread to the

bottom of the vessel containing the mercury. When the magnet was thus

floating almost vertically with its north pole above the surface, a

current of positive electricity was made to descend perpendicularly

through a wire touching the mercury, and immediately the magnet began to

rotate from left to right about the wire. The force being uniform, the

rotation was accelerated till the tangential force was balanced by the

resistance of the mercury, when it became constant. Under the same

circumstances the south pole of the magnet rotates from right to left.

It is evident, from this experiment, that the wire may also be made to

perform a rotation round the magnet, since the action of the current of

electricity on the pole of the magnet must necessarily be accompanied by

a corresponding reaction of the pole of the magnet on the electricity in

the wire. This experiment has been accomplished by a vast number of

contrivances, and even a small battery, consisting of two plates, has

performed the rotation. Dr. Faraday produced both motions at the same

time in a vessel containing mercury; the wire and the magnet revolved in

one direction about a common centre of motion, each following the other.

The next step was to make a magnet, and also a cylinder, revolve about

their own axes, which they do with great rapidity. Mercury has been made

to rotate by means of Voltaic electricity, and Professor Ritchie

exhibited in the Royal Institution the singular spectacle of the

rotation of water by the same means, while the vessel containing it

remained stationary. The water was in a hollow double cylinder of glass,

and, on being made the conductor of electricity, was observed to revolve

in a regular vortex, changing its direction as the poles of the battery

were alternately reversed. Professor Ritchie found that all the

different conductors hitherto tried by him, such as water, charcoal,

&c., give the same electro-magnetic results when transmitting the same

quantity of electricity, and that they deflect the magnetic needle in an

equal degree when their respective axes of conduction are at the same

distance from it. But one of the most extraordinary effects of this

force is exhibited by coiling a copper wire, so as to form a helix or

corkscrew, and connecting the extremities of the wire with the poles of

a galvanic battery. If a magnetized steel bar or needle be placed within

the screw, so as to rest upon the lower part, the instant a current of

electricity is sent through the wire of the helix, the steel bar starts

up by the influence of this invisible power, and remains suspended in

the air in opposition to the force of gravitation (N. 224). The effect

of the electro-magnetic power exerted by each turn of the wire is to

urge the north pole of the magnet in one direction, and the south pole

in the other. The force thus exerted is multiplied in degree and

increased in extent by each repetition of the turns of the wire, and in

consequence of these opposing forces the bar remains suspended. This

helix has all the properties of a magnet while the electrical current is

flowing through it, and may be substituted for one in almost every

experiment. It acts as if it had a north pole at one extremity and a

south pole at the other, and is attracted and repelled by the poles of a

magnet exactly as if it were one itself. All these results depend upon

the course of the electricity; that is, on the direction of the turns of

the screw, according as it is from right to left, or from left to right,

being contrary in the two cases.

The action of Voltaic electricity on a magnet is not only precisely the

same with the action of two magnets on one another, but its influence in

producing temporary magnetism in iron and steel is also the same with

magnetic induction. The term induction, when applied to electric

currents, expresses the power which these currents possess of inducing a

particular state upon matter in their immediate neighbourhood, otherwise

neutral or indifferent. For example, the connecting wire of a galvanic

battery holds iron filings suspended like a magnet as long as the

current continues to flow through it: the iron becomes magnetic by the

induction of the current. The most powerful temporary magnets are

obtained by bending a thick cylinder of soft iron into the form of a

horseshoe, and surrounding it with a coil of thick copper wire covered

with silk to prevent communication between its coils. When this wire

forms part of a galvanic circuit the iron becomes so highly magnetic by

the induction of the current flowing through the wire that a temporary

magnet of this kind made by Professor Henry of the Albany Academy in the

United States sustained a weight of nearly a ton. Another by Mr. Gage

has been applied with considerable success as a moving power: its spark

is a bright flash, and the snap as loud as a pistol. But the most

powerful known is that employed by Mr. Joule in his experiments, which

sustains a weight of 2080 lbs. The iron loses its magnetism the instant

the electricity ceases to flow, and acquires it again as instantaneously

when the circuit is renewed.

The action of an electric current causes a deviation of the compass from

the plane of the magnetic meridian. In proportion as the needle recedes

from the meridian, the intensity of the force of terrestrial magnetism

increases, while at the same time the electro-magnetic force diminishes;

the number of degrees at which the needle stops, showing where the

equilibrium between these two forces takes place, will indicate the

intensity of the galvanic current. The galvanometer, constructed upon

this principle, is employed to measure the intensity of galvanic

currents collected and conveyed to it by wires. This instrument is

rendered much more sensible by neutralizing the effects of the earth’s

magnetism on the needle, which is accomplished by placing a second

magnetised needle so as to counteract the action of the earth on the

first—a precaution requisite in all delicate magnetical experiments.

It has been ascertained by means of this instrument that the action of

an electrical current upon a magnet is inversely as the square of the

distance, and the energy with which an electro magnet acts is directly

as the power of the galvanic battery and the number of coils round the

core, and inversely as the resistance of the wire.

On the Connexion of the Physical Sciences · 第 30 / 39 章