Step 1: Understand the concept
The changing current in P induces an emf in S: \(\varepsilon_S = M\dfrac{dI_p}{dt}\). The secondary has resistance and self inductance, so its current is limited by its impedance.
Step 2: Maximum emf
\(I_p = 12\sin(50\pi t)\), so \(\dfrac{dI_p}{dt} = 600\pi\cos(50\pi t)\) with peak \(600\pi\) A/s. With \(M = \pi\times10^{-3}\) H:
\[ \varepsilon_{max} = \pi\times10^{-3}\times600\pi = 0.6\pi^2 = 6\ \text{V} \]
Step 3: Impedance of S
Reactance \(X_L = \omega L = 50\pi\times\dfrac{60}{\pi}\times10^{-3} = 3\ \Omega\). Resistance is \(4\ \Omega\), so \(Z = \sqrt{4^2 + 3^2} = 5\ \Omega\).
Step 4: Maximum current
\[ I_{max} = \frac{6}{5} = 1.2\ \text{A} \]
Option (D). If the self inductance were ignored, we would get \(\frac{6}{4} = 1.5\) A, which is option (C) and is a trap.
Final Answer:
The maximum induced current is 1.2 A. This is option (D).
\[ \boxed{\text{(D) }1.2\ \text{A}} \]