Step 1: Recall induced emf for rotating coil.
\[
\varepsilon_{\text{rms}} = N A B \omega / \sqrt{2}
\]
Step 2: Substitute known values.
\[
N = 40, \, A = 0.01 \, \text{m}^2, \, B = 0.05 \, \text{T}, \, \omega = 50 \, \text{rad/s}
\]
\[
\varepsilon_{\text{rms}} = \frac{40 \cdot 0.01 \cdot 0.05 \cdot 50}{\sqrt{2}} \approx 0.707 \, \text{V}
\]
Step 3: Recall power in resistor.
\[
P = \frac{\varepsilon_{\text{rms}}^2}{R} \implies R = \frac{\varepsilon_{\text{rms}}^2}{P}
\]
Step 4: Substitute power.
\[
P = 25 \, \text{mW} = 0.025 \, \text{W}
\]
\[
R = \frac{0.707^2}{0.025} \approx 20 \, \Omega
\]
Step 5: Verify reasoning.
RMS emf formula correct for rotation about diameter; power formula consistent.
Step 6: Final conclusion.
Hence, the closed loop resistance of the coil is:
\[
\boxed{20 \, \Omega}
\]