The problem asks for the ratio of the moment of inertia ($I_1$) of a solid cylinder to that ($I_2$) of a smaller, co-centric cylinder carved from it.
The moment of inertia ($I$) for a uniform solid cylinder of mass $M$ and radius $R$ about its central axis is given by the formula:
$I = \frac{1}{2}MR^2$
We assume the original cylinder has uniform density ($\rho$). The mass ($M$) can be expressed as $M = \rho V$, where $V$ is the volume. For a cylinder, $V = \pi R^2 L$. Thus, $M = \rho \pi R^2 L$. Substituting this into the inertia formula gives:
$I = \frac{1}{2}(\rho \pi R^2 L)R^2 = \frac{1}{2}\rho \pi R^4 L$
For the original solid cylinder:
For the smaller carved cylinder:
Now, we find the ratio of the moments of inertia:
$ \frac{I_1}{I_2} = \frac{\frac{1}{2}\rho \pi R^4 L}{\frac{1}{2} \left(\frac{1}{162} \rho \pi R^4 L\right)} $
Cancel out the common terms ($\frac{1}{2}\rho \pi R^4 L$):
$ \frac{I_1}{I_2} = \frac{1}{\frac{1}{162}} = 162 $
The ratio $I_1/I_2$ is 162.
In the given figure the blocks $A$, $B$ and $C$ weigh 4 kg, 6 kg and 8 kg respectively. The co-efficient of sliding friction between any two surfaces is 0.5. The force $\vec{F}$ required to slide the block $C$ with constant speed is ______ N. (Use $g = 10 \text{ m/s}^2$)

A thin uniform rod ($X$) of mass $M$ and length $L$ is pivoted at a height $\left(\frac{L}{3}\right)$ as shown in the figure. The rod is allowed to fall from a vertical position and lie horizontally on the table. The angular velocity of this rod when it hits the table top, is __________.
($g = \text{gravitational acceleration}$)

In the given figure the blocks $A$, $B$ and $C$ weigh 4 kg, 6 kg and 8 kg respectively. The co-efficient of sliding friction between any two surfaces is 0.5. The force $\vec{F}$ required to slide the block $C$ with constant speed is ______ N. (Use $g = 10 \text{ m/s}^2$)
