Page:A Treatise on Electricity and Magnetism - Volume 2.djvu/391

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759.]
KIRCHHOFF'S METHOD.
359

from and placed in a position in which the coefficient of mutual induction between and is zero (Art. 538), a current of induction is produced in both circuits, and the galvanometer needle receives an impulse which produces a certain transient deflexion.

The resistance of the wire, , is deduced from a comparison between the permanent deflexion, due to the steady current, and the transient deflexion, due to the current of induction.

Let the resistance of be , of , , and of , .

Let , and be the coefficients of induction of and .

Let be the current in , and that in , then the current from to is .

Let be the electromotive force of the battery, then


,(1)

.(2)


When the currents are constant, and everything at rest,


.(3)


If now suddenly becomes zero on account of the separation of from , then, integrating with respect to ,


,(4)

.(5)
whence .(6)


Substituting the value of in terms of from (3), we find

��x M

x~ R *

When, as in Kirchhoff's experiment, both and are large compared with , this equation is reduced to


.(9)


Of these quantities, is found from the throw of the galvanometer due to the induction current. See Art. 768. The permanent current, , is found from the permanent deflexion due to the steady current; see Art. 746. is found either by direct calculation from the geometrical data, or by a comparison with a pair of coils, for which this calculation has been made; see Art. 755. From