Let the acceleration of sphere A be \(a_A\) and the acceleration of sphere B be \(a_B\).
For rolling motion, we know that the force applied causes both linear and rotational acceleration. The relation between the linear and rotational acceleration for rolling objects is given by:
\[
F = ma + I \alpha
\]
where \(m\) is the mass, \(a\) is the linear acceleration, \(I\) is the moment of inertia, and \(\alpha\) is the angular acceleration.
For both spheres, the condition for rolling without slipping is:
\[
a = R \alpha
\]
For solid sphere (A):
- Moment of inertia \(I_A = \frac{2}{5}mR^2\)
- Using \(F = ma_A + I_A \alpha_A\) and \(a_A = R \alpha_A\), we get:
\[
F = m a_A + \frac{2}{5} m R^2 \frac{a_A}{R}
\]
\[
F = m a_A \left(1 + \frac{2}{5}\right)
\]
\[
F = \frac{7}{5} m a_A
\]
\[
a_A = \frac{5}{7} \frac{F}{m}
\]
For hollow sphere (B):
- Moment of inertia \(I_B = \frac{2}{3}mR^2\)
- Using \(F = ma_B + I_B \alpha_B\) and \(a_B = R \alpha_B\), we get:
\[
F = m a_B + \frac{2}{3} m R^2 \frac{a_B}{R}
\]
\[
F = m a_B \left(1 + \frac{2}{3}\right)
\]
\[
F = \frac{5}{3} m a_B
\]
\[
a_B = \frac{3}{5} \frac{F}{m}
\]
Step 3: Find the ratio of accelerations:
\[
\frac{a_A}{a_B} = \frac{\frac{5}{7} \frac{F}{m}}{\frac{3}{5} \frac{F}{m}} = \frac{5}{7} \times \frac{5}{3} = \frac{25}{21} \approx \frac{10}{21}
\]
Thus, the ratio of the accelerations is \(\frac{10}{21}\).
Final Answer: Option (B) \(\frac{10}{21}\).