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, \( a = \dfrac{F}{2m} \)
The left and right compartments of a thermally isolated container of length $L$ are separated by a thermally conducting, movable piston of area $A$. The left and right compartments are filled with $\frac{3}{2}$ and 1 moles of an ideal gas, respectively. In the left compartment the piston is attached by a spring with spring constant $k$ and natural length $\frac{2L}{5}$. In thermodynamic equilibrium, the piston is at a distance $\frac{L}{2}$ from the left and right edges of the container as shown in the figure. Under the above conditions, if the pressure in the right compartment is $P = \frac{kL}{A} \alpha$, then the value of $\alpha$ is ____
Let $ S $ denote the locus of the point of intersection of the pair of lines $$ 4x - 3y = 12\alpha,\quad 4\alpha x + 3\alpha y = 12, $$ where $ \alpha $ varies over the set of non-zero real numbers. Let $ T $ be the tangent to $ S $ passing through the points $ (p, 0) $ and $ (0, q) $, $ q > 0 $, and parallel to the line $ 4x - \frac{3}{\sqrt{2}} y = 0 $.
Then the value of $ pq $ is