Step 1: Field at the centre:
The big coil (radius \(r_1\), one turn) carries a current I and produces a field at the centre \(B = \frac{\mu_0I}{2r_1}\).
Step 2: Flux through the small coil:
Since \(r_2 \ll r_1\), the field is nearly uniform over the small coil: \(\Phi = B\cdot\pi r_2^2 = \frac{\mu_0I\,\pi r_2^2}{2r_1}\).
Step 3: Mutual inductance:
\[ M = \frac\Phi I = \frac{\mu_0\pi r_2^2}{2r_1} \]
Final Answer:
The mutual inductance is \(\frac{\mu_0\pi r_2^2}{2r_1}\), option (D).
\[ \boxed{M = \frac{\mu_0 \pi r_2^2}{2r_1}} \]