Step 1: Understanding the concept of mutual induction
The emf induced in the second coil due to mutual inductance is given by:
\[
e = M \frac{dI}{dt}
\]
where:
- \( M \) is the mutual inductance,
- \( \frac{dI}{dt} \) is the rate of change of current in the first coil.
Step 2: Differentiate the given current equation
The given current equation is:
\[
I = 12 \sin 100t
\]
Differentiating with respect to \( t \):
\[
\frac{dI}{dt} = 12 \times 100 \cos 100t
\]
\[
= 1200 \cos 100t
\]
Step 3: Compute maximum induced emf
The maximum emf occurs when \( \cos 100t = 1 \), so:
\[
\left( \frac{dI}{dt} \right)_{\max} = 1200
\]
Given \( M = 8 \) mH = \( 8 \times 10^{-3} \) H, the maximum induced emf is:
\[
e_{\max} = M \times 1200
\]
\[
= (8 \times 10^{-3}) \times 1200
\]
\[
= 9.6 \text{ V}
\]
Thus, the maximum induced emf in the second coil is \( 9.6 \) V.
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