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Page:A Treatise on Electricity and Magnetism - Volume 2.djvu/386

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354
COMPARISON OF COILS.
754.]

We have then, by Art. 276,]

γR1 =(γγ)R2, (3)
or γγ =R1+R2R2, (4)
and G1 =R1+R2R2G1. (5)

If there is any uncertainty about the actual resistance of the galvanometer coil (on account, say, of an uncertainty as to its temperature) we may add resistance coils to it, so that the resistance of the galvanometer itself forms but a small part of R1, and thus introduces but little uncertainty into the final result.

754.] To determine g1, the magnetic moment of a small coil due to a unit-current flowing through it, the magnet is still suspended at the centre of the standard coil, but the small coil is moved parallel to itself along the common axis of both coils, till the same current, flowing in opposite directions round the coils, no longer deflects the magnet. If the distance between the centres of the coils is r, we have now

G1=2g1r3+3g2r4+4g3r5+&c.
(6)

By repeating the experiment with the small coil on the opposite side of the standard coil, and measuring the distance between the positions of the small coil, we eliminate the uncertain error in the determination of the position of the centres of the magnet and of the small coil, and we get rid of the terms in g2, g4, &c.

If the standard coil is so arranged that we can send the current through half the number of windings, so as to give a different value to G1, we may determine a new value of r, and thus, as in Art. 454, we may eliminate the term involving g3.

It is often possible, however, to determine g3 by direct measurement of the small coil with sufficient accuracy to make it available in calculating the value of the correction to be applied to g1 in the equation

g1=12G1r32g3r2.
(7)
where
g3=18πa2(6a2+3ξ22η2), by Art. 700.


Comparison of Coefficients of Induction.

755.] It is only in a small number of cases that the direct calculation of the coefficients of induction from the form and