348 STANDARD ELECTRICAL DICTIONARY.

Magnetic Intensity.

The intensity of the magnetization of a body. It is measured by the

magnetic lines of force passing through a unit area of the body, such

area being at right angles to the direction of the lines of force.

Magnetic Lag.

In magnetism the tendency of hard iron or steel especially to take up

magnetism slowly, and to part with it slowly. (See Magnetic Inertia.)

The lag affects the action of a dynamo, and is a minor cause of those

necessitating the lead of the brushes.

Synonym--Magnetic Retardation.

Magnetic Latitude.

Latitude referred to the magnetic equator and isoclinic lines.

Magnetic Leakage.

The lines of force in a field magnet which pass through the air and not

through the armature are useless and represent a waste of field. Such

lines constitute magnetic leakage.

Magnetic Limit.

The temperature beyond which a paramagnetic metal cannot be magnetized.

The magnetic limit of iron is from a red to a white heat; of cobalt, far

beyond a white heat; of chromium, below a red heat; of nickel at about

350° C. (662°F.) of manganese, from 15° C. to 20° C. (59° to 68° F.)

Magnetic Lines of Force.

Lines of force indicating the distribution of magnetic force, which is

due presumably to whirls of the ether. A wire or conductor through which

a current is passing is surrounded by an electro-magnetic field of

force, q. v., whose lines of force form circles surrounding the

conductor in question. A magnet marks the existence of a similar

electro-magnetic field of force whose lines form circuits comprising

part of and in some places all of the body of the magnet, and which are

completed through the air or any surrounding paramagnetic or diamagnetic

body. They may be thought of as formed by the Ampérian sheet of current,

and analogous to those just mentioned as surrounding a conductor.

Fig. 223. MAGNETIC LINES OF FORCE, DIRECTION OF.

A magnetic line of force may be thought of as a set of vortices or

whirls, parallel to each other, and strung along the line of force which

is the locus of their centres.

If as many lines are drawn per square centimeter as there are dynes (per

unit pole) of force at the point in question, each such line will be a

unitary c. g. s. line of force.

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