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Question
Find the mutual inductance between the circular coil and the loop shown in figure.

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Solution

The magnetic field due to coil 1 at the centre of coil 2 is given by
\[B = \frac{\mu_0 Ni a^2}{2 ( a^2 + x^2 )^{3/2}}\]
The flux linked with coil 2 is given by
\[\phi = B . A' = \frac{\mu_0 Ni a^2}{2 ( a^2 + x^2 )^{3/2}}\pi a '^2\]
Now, let y be the distance of the sliding contact from its left end.
Given:-
\[v = \frac{dy}{dt}\]
Total resistance of the rheostat = R
When the distance of the sliding contact from the left end is y, the resistance of the rheostat is given by
\[r' = \frac{R}{L}y\]
The current in the coil is the function of distance y travelled by the sliding contact of the rheostat. It is given by
\[i = \frac{E}{\left( \frac{R}{L}y + r \right)}\]
The magnitude of the emf induced can be calculated as:-
\[e = \frac{d\phi}{dt} = \frac{\mu_0 N a^2 a '^2 \pi}{2 ( a^2 + x^2 )^{3/2}}\frac{di}{dt}\]
\[e = \frac{\mu_0 N \pi a^2 a '^2}{2 ( a^2 + x^2 )^{3/2}}\frac{d}{dt}\frac{E}{\left( \frac{R}{L}y + r \right)}\]
\[e = \frac{\mu_0 N \pi a^2 a '^2}{2 ( a^2 + x^2 )^{3/2}}\left[ E\frac{\left( - \frac{R}{L}v \right)}{\left( \frac{R}{L}y + r \right)^2} \right]\]
emf induced,
\[e = \frac{\mu_0 N \pi a^2 a '^2}{2 ( a^2 + x^2 )^{3/2}}\left[ E\frac{\left( - \frac{R}{L}v \right)}{\left( \frac{R}{L}y + r \right)^2} \right]\]
The emf induced in the coil can also be given as:-
\[\frac{di}{dt} = \left[ E\frac{\left( - \frac{R}{L}v \right)}{\left( \frac{R}{L}y + r \right)^2} \right]\]
\[e = M\frac{di}{dt} , \frac{di}{dt} = \left[ E\frac{\left( - \frac{R}{L}v \right)}{\left( \frac{R}{L}y + r \right)^2} \right]\]
\[M = \frac{e}{\frac{di}{dt}} = \frac{N \mu_0 \pi a^2 a '^2}{2( a^2 + x^2 )^{3/2}}\]
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