358 STANDARD ELECTRICAL DICTIONARY.

Magnetic Remanence.

The residual magnetism left in a bar of steel or other paramagnetic

material after the application of a powerful magnet. It is distinguished

from coercive force, as the latter is the amount of negative magnetizing

or of demagnetizing force required to reduce the remanent magnetism to

zero.

Synonym--Remanence--Residual Magnetism.

Magnetism, Solenoidal Distribution of.

The distribution of magnetism in such a way that the poles are very far

apart in proportion to their area. The magnetization of a long thin bar

of steel illustrates solenoidal distribution.

Magnetism Sub-permanent.

The magnetism of a paramagnetic substance which presents a considerable

degree of permanency, but which gradually disappears, leaving the

permanent magnetism present. It is noticeable in iron or steel ships

whose magnetism gradually reduced in quantity, eventually becomes fully

permanent.

Magnetism, Weber's Theory of.

The molecules of a magnetizable material by this theory are supposed to

be magnets with their poles lying in every direction, and hence

neutralizing each other. By magnetization these are supposed to be

turned with their similar poles in the same direction, and their axis

parallel, hence acting like a group of magnets. It is practically

identical with Hughes' theory.

Magnetism, Terrestrial.

The magnetism of the earth. (See Magnetic Elements.)

Fig. 228. MAGNETIZATION BY DOUBLE TOUCH.

Magnetization by Double Touch.

The process of magnetizing a steel bar by simultaneously stroking it

with two poles of a horseshoe magnet or with two opposite poles of two

bar magnets. The poles must be close but not touching. A block of wood

may be placed between the ends if single magnets are used. The poles are

placed on the middle of the bar and carried back and forth to one end,

then to the other, and so on, ending at the middle of the bar in such

direction as to give each end the same number of strokes. The poles must

be close together or consequent poles will be produced. If bar magnets

are used they may be held inclined at an angle of 15º to 20º with the

horizontal bar to be magnetized. The ends of the latter may rest on

poles of two other magnets, each end on a pole of the same name as that

of the magnetizing magnet on its side. (See Magnetization, Hoffer's

Method.)

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