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