Step 1: Understanding the problem.
The torque required to rotate the disc is related to the moment of inertia \( I \) and the angular acceleration \( \alpha \). The moment of inertia of a solid disc is given by:
\[
I = \frac{1}{2} MR^2
\]
The angular acceleration \( \alpha \) is related to the angular velocity \( \omega \) and the time \( t \) by the equation:
\[
\alpha = \frac{\omega}{t}
\]
The tangential force \( F \) applied at the rim of the disc is related to the torque \( \tau \) by:
\[
\tau = F R = I \alpha
\]
Substituting \( I = \frac{1}{2} MR^2 \) and \( \alpha = \frac{\omega}{t} \), we get:
\[
F R = \frac{1}{2} MR^2 \cdot \frac{\omega}{t}
\]
Solving for \( F \), we find:
\[
F = \frac{MR \omega}{2t}
\]
Step 2: Conclusion.
The tangential force required to rotate the disc is \( \frac{MR \omega}{2t} \). Therefore, the correct answer is option (C).