Concept:
The total magnetic flux linkage through a secondary inductor coil ($\phi_s$) due to a current passing in the primary loop ($I_p$) is related by the mutual inductance factor $M$:
\[
N_s \phi_s = M I_p
\]
According to Faraday's law of electromagnetic induction, the magnitude of the electromotive force (emf) induced in the secondary inductor as the primary current changes over time is:
\[
e_s = M \frac{dI_p}{dt}
\]
Step 1: Determine the mutual inductance ($M$).
We are given the following values:
• Primary current, $I_p = 2.5\text{ A}$
• Secondary turns, $N_s = 400$
• Flux through a single secondary turn, $\phi_s = 600 \times 10^{-6}\text{ T m}^2$
• Rate of change of primary current, $\frac{dI_p}{dt} = 0.2\text{ A s}^{-1}$
Using the flux linkage relation to isolate $M$:
\[
M = \frac{N_s \phi_s}{I_p}
\]
\[
M = \frac{400 \times 600 \times 10^{-6}}{2.5} = \frac{240000 \times 10^{-6}}{2.5} = 96000 \times 10^{-6} = 0.096\text{ H}
\]
Step 2: Calculate the induced secondary emf ($e_s$).
Using Faraday's statement:
\[
e_s = M \frac{dI_p}{dt}
\]
\[
e_s = 0.096 \times 0.2 = 0.0192\text{ V} = 1.92 \times 10^{-2}\text{ V}
\]