A uniform hollow cylinder is a cylindrical shell characterized by having both an inner and an outer radius. To find the moment of inertia \( I \) of the hollow cylinder about its axis, we integrate across the volume of the cylindrical shell. The moment of inertia for a differential mass element \( dm \) at a distance \( r \) from the axis is given by \( dI = r^2 \, dm \).
The volume of the hollow cylinder is determined by subtracting the volume of the inner cylinder from the volume of the outer cylinder:
\[ V = \pi b^2 L - \pi a^2 L = \pi (b^2 - a^2) L \]
Given the density \( \rho \), the mass \( M \) of the hollow cylinder can be expressed as:
\[ M = \rho V = \rho \pi (b^2 - a^2) L \]
For a small ring element at radius \( r \), the differential area \( dA \) is the area of the ring: \( dA = 2\pi r \, dr \), and thus the differential volume of the ring \( dV = 2\pi r L \, dr \).
The differential mass is:
\[ dm = \rho \, dV = \rho (2\pi r L \, dr) \]
To find the moment of inertia of the entire cylinder, integrate over the thickness of the shell from \( a \) to \( b \):
\[ I = \int_{a}^{b} r^2 \, dm = \int_{a}^{b} r^2 \rho (2\pi r L \, dr) = 2\pi \rho L \int_{a}^{b} r^3 \, dr \]
The definite integral \( \int_{a}^{b} r^3 \, dr \) evaluates to:
\[ \int_{a}^{b} r^3 \, dr = \left[\frac{r^4}{4}\right]_{a}^{b} = \frac{b^4}{4} - \frac{a^4}{4} \]
Plug this result back into the expression for \( I \):
\[ I = 2\pi \rho L \left(\frac{b^4 - a^4}{4}\right) \]
Simplifying gives:
\[ I = \frac{\pi \rho L (b^4 - a^4)}{2} \]
Substituting \( M = \rho \pi (b^2 - a^2) L \), which implies \( \rho = \frac{M}{\pi (b^2 - a^2) L} \), we can write:
\[ I = \frac{M}{2} \frac{b^4 - a^4}{b^2 - a^2} \]
Notice that:
\[ \frac{b^4 - a^4}{b^2 - a^2} = (b^2 + a^2) \] (by polynomial identity)
So, finally:
\[ I = \frac{M}{2} (b^2 + a^2) \]
The correct answer is therefore \[ M(b^2 + a^2) \].
If $\overrightarrow{\mathrm{L}}$ and $\overrightarrow{\mathrm{P}}$ represent the angular momentum and linear momentum respectively of a particle of mass ' $m$ ' having position vector $\overrightarrow{\mathrm{r}}=\mathrm{a}(\hat{\mathrm{i}} \cos \omega \mathrm{t}+\hat{\mathrm{j}} \sin \omega \mathrm{t})$. The direction of force is
A uniform circular disc of radius \( R \) and mass \( M \) is rotating about an axis perpendicular to its plane and passing through its center. A small circular part of radius \( R/2 \) is removed from the original disc as shown in the figure. Find the moment of inertia of the remaining part of the original disc about the axis as given above.
Which of the following are correct expression for torque acting on a body?
A. $\ddot{\tau}=\ddot{\mathrm{r}} \times \ddot{\mathrm{L}}$
B. $\ddot{\tau}=\frac{\mathrm{d}}{\mathrm{dt}}(\ddot{\mathrm{r}} \times \ddot{\mathrm{p}})$
C. $\ddot{\tau}=\ddot{\mathrm{r}} \times \frac{\mathrm{d} \dot{\mathrm{p}}}{\mathrm{dt}}$
D. $\ddot{\tau}=\mathrm{I} \dot{\alpha}$
E. $\ddot{\tau}=\ddot{\mathrm{r}} \times \ddot{\mathrm{F}}$
( $\ddot{r}=$ position vector; $\dot{\mathrm{p}}=$ linear momentum; $\ddot{\mathrm{L}}=$ angular momentum; $\ddot{\alpha}=$ angular acceleration; $\mathrm{I}=$ moment of inertia; $\ddot{\mathrm{F}}=$ force; $\mathrm{t}=$ time $)$
Choose the correct answer from the options given below:
A wheel of radius $ 0.2 \, \text{m} $ rotates freely about its center when a string that is wrapped over its rim is pulled by a force of $ 10 \, \text{N} $. The established torque produces an angular acceleration of $ 2 \, \text{rad/s}^2 $. Moment of inertia of the wheel is............. kg m².
A tube of length 1m is filled completely with an ideal liquid of mass 2M, and closed at both ends. The tube is rotated uniformly in horizontal plane about one of its ends. If the force exerted by the liquid at the other end is \( F \) and the angular velocity of the tube is \( \omega \), then the value of \( \alpha \) is ______ in SI units.