In rotational motion, the work done \( W \) by a constant torque \( \tau \) is given by:
\[
W = \tau \theta,
\]
where:
- \( \tau \) is the constant torque (10 Nm),
- \( \theta \) is the angular displacement.
Step 1: Find angular displacement
Since the body starts from rest and is rotated for 25 seconds under a constant moment of force (torque), we can use the equation for angular displacement under constant angular acceleration:
\[
\theta = \omega_0 t + \frac{1}{2} \alpha t^2,
\]
where:
- \( \omega_0 \) is the initial angular velocity (which is 0 since the body starts from rest),
- \( t \) is the time (25 s),
- \( \alpha \) is the angular acceleration.
Since \( \tau = I \alpha \) (where \( I \) is the moment of inertia), the angular acceleration is:
\[
\alpha = \frac{\tau}{I}.
\]
Substituting \( \tau = 10 \, \text{Nm} \) and \( I = 5 \, \text{kg m}^2 \), we get:
\[
\alpha = \frac{10}{5} = 2 \, \text{rad/s}^2.
\]
Now, substitute \( \alpha = 2 \, \text{rad/s}^2 \) and \( t = 25 \, \text{s} \) into the equation for \( \theta \):
\[
\theta = 0 \times 25 + \frac{1}{2} \times 2 \times 25^2 = \frac{1}{2} \times 2 \times 625 = 625 \, \text{rad}.
\]
Step 2: Calculate the work done
Now, substitute the values of \( \tau \) and \( \theta \) into the work equation:
\[
W = 10 \times 625 = 6250 \, \text{J}.
\]
Thus, the work done is 6250 J, which corresponds to option (C).