The moment of inertia of a solid sphere about its diameter is given by the formula:
\( I_{\text{sphere}} = \frac{2}{5}mr^2 \)
where: - \( m \) is the mass of the sphere, - \( r \) is the radius of the sphere.
The parallel axis theorem states that the moment of inertia of a body about an axis parallel to and a distance \( d \) away from an axis through its center of mass is given by:
\( I = I_{\text{cm}} + md^2 \)
where: - \( I_{\text{cm}} \) is the moment of inertia about the center of mass axis, - \( d \) is the distance from the center of mass to the new axis.
The distance between the center of a sphere and the midpoint of the rod is:
\( d = \frac{40}{2} \, \text{cm} = 20 \, \text{cm} = 0.2 \, \text{m} \)
The radius of each sphere is \( r = 10 \, \text{cm} = 0.1 \, \text{m} \). Using the parallel axis theorem, the moment of inertia of one sphere about the midpoint of the rod is:
\( I_{\text{one}} = \frac{2}{5}mr^2 + md^2 \)
Substitute the values into the equation:
\( I_{\text{one}} = \frac{2}{5}(2)(0.1)^2 + (2)(0.2)^2 = 0.008 + 0.08 = 0.088 \, \text{kg-m}^2 \)
Since there are two identical spheres, the total moment of inertia of the system is:
\( I_{\text{sys}} = 2 \times I_{\text{one}} = 2 \times 0.088 = 0.176 \, \text{kg-m}^2 = 176 \times 10^{-3} \, \text{kg-m}^2 \)
The moment of inertia of the system is \( \mathbf{176 \times 10^{-3} \, \text{kg-m}^2} \).
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.

Let \( a \in \mathbb{R} \) and \( A \) be a matrix of order \( 3 \times 3 \) such that \( \det(A) = -4 \) and \[ A + I = \begin{bmatrix} 1 & a & 1 \\ 2 & 1 & 0 \\ a & 1 & 2 \end{bmatrix} \] where \( I \) is the identity matrix of order \( 3 \times 3 \).
If \( \det\left( (a + 1) \cdot \text{adj}\left( (a - 1) A \right) \right) \) is \( 2^m 3^n \), \( m, n \in \{ 0, 1, 2, \dots, 20 \} \), then \( m + n \) is equal to: