
Given:
Important condition: No slipping means the point of contact has zero relative velocity, hence:
\[ a = R \alpha \quad \text{(where } \alpha \text{ is angular acceleration)} \]
Translational motion:
Net force on the center of mass:
\[
F - f = m a \tag{1}
\]
Rotational motion about center:
\[
f R = I \alpha \Rightarrow f R = I \cdot \frac{a}{R} \tag{2}
\]
For a thin-walled hollow cylinder:
Moment of inertia about the center is:
\[
I = m R^2
\]
Substituting in equation (2):
\[
f R = m R^2 \cdot \frac{a}{R} \Rightarrow f = m a \tag{3}
\]
Now substitute (3) into (1): \[ F - m a = m a \Rightarrow F = 2 m a \Rightarrow a = \frac{F}{2m} \]
β Correct Answer: Option (D): For a thin-walled hollow cylinder, \( a = \dfrac{F}{2m} \)
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