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A conducting loop of resistance ' $R$ ' is moved into a magnetic field, the total induced charge depends upon
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the total change in magnetic flux and $\mathrm{R}$.
$\begin{aligned} & \mathrm{i}=\frac{\mathrm{e}}{\mathrm{R}}=\frac{1}{\mathrm{R}} \cdot \frac{\Delta \phi}{\Delta \mathrm{t}} \\ & \frac{\Delta \mathrm{q}}{\Delta \mathrm{t}}=\frac{1}{\mathrm{R}} \cdot \frac{\Delta \phi}{\Delta \mathrm{t}} \\ & \therefore \Delta \mathrm{q}=\frac{\Delta \phi}{\mathrm{R}}\end{aligned}$
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