A short bar magnet placed with its axis at \( 30^\circ \) and a uniform external magnetic field of 0.5 T experiences a torque of magnitude equal to \( 4.5 \times 10^{-2} \) J. Then the magnitude of the magnetic moment of the magnet will be
Step 1: Understanding Magnetic Torque
- The torque (\(\tau\)) experienced by a magnetic dipole in a uniform magnetic field is given by: \[ \tau = MB \sin \theta \] where:
- \( M \) is the magnetic moment of the magnet, - \( B \) is the external magnetic field strength, - \( \theta \) is the angle between the magnetic moment and the field.
Step 2: Given Values
- \( \tau = 4.5 \times 10^{-2} \) J, - \( B = 0.5 \) T, - \( \theta = 30^\circ \), - \(\sin 30^\circ = \frac{1}{2} \).
Step 3: Calculating \( M \)
Rearranging the equation: \[ M = \frac{\tau}{B \sin \theta} \] \[ M = \frac{4.5 \times 10^{-2}}{(0.5) \times (\frac{1}{2})} \] \[ M = \frac{4.5 \times 10^{-2}}{0.25} \] \[ M = 18 \times 10^{-2} \] \[ M = 18 \times 10^{-2} { J T}^{-1} \] Thus, the magnetic moment of the magnet is \( 18 \times 10^{-2} \) J T\(^{-1}\).
A block of certain mass is placed on a rough floor. The coefficients of static and kinetic friction between the block and the floor are 0.4 and 0.25 respectively. A constant horizontal force \( F = 20 \, \text{N} \) acts on it so that the velocity of the block varies with time according to the following graph. The mass of the block is nearly (Take \( g = 10 \, \text{m/s}^2 \)):
If the value of \( \cos \alpha \) is \( \frac{\sqrt{3}}{2} \), then \( A + A = I \), where \[ A = \begin{bmatrix} \sin\alpha & -\cos\alpha \\ \cos\alpha & \sin\alpha \end{bmatrix}. \]