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The total emf induced in a closely would coil of $\mathrm{N}$ turns in which the magnetic flux linked with the coil changing at the rate $\frac{\mathrm{d} \phi_{\mathrm{B}}}{\mathrm{dt}}$ is
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$-\mathrm{N} \frac{\mathrm{d} \phi_{\mathrm{B}}}{\mathrm{dt}}$
For a coil of $\mathrm{N}$ turns, the emf across the whole coil is $\varepsilon=-\mathrm{N} \frac{\mathrm{d} \phi_{\mathrm{B}}}{\mathrm{dt}}$
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