The induced potential difference \( V \) in a rotating conducting disc is given by:
\[
V = \frac{1}{2} B \omega R^2
\]
where:
- \( B = 0.4 \) T (magnetic field strength),
- \( \omega = 10\pi \) rad/s (angular velocity),
- \( R = 20 \) cm \( = 0.2 \) m (radius of the disc).
Substituting the values:
\[
V = \frac{1}{2} \times 0.4 \times 10\pi \times (0.2)^2
\]
\[
V = \frac{1}{2} \times 0.4 \times 10\pi \times 0.04
\]
\[
V = \frac{1}{2} \times 0.4 \times 0.4\pi
\]
\[
V = \frac{1}{2} \times 0.16\pi
\]
\[
V = 0.08\pi
\]
Since \( \pi = 3.14 \), we calculate:
\[
V = 0.08 \times 3.14 = 0.2512 { V}
\]
Thus, the correct answer is (2) 0.2512 V.