The magnetic dipole moment \( \vec{m} \) of a current loop is given by: \[ \vec{m} = I \cdot A \cdot \hat{n} \] Where: - \( I = 2 \, \text{A} \) is the current, - \( A = \pi r^2 \) is the area of the loop, and - \( \hat{n} \) is the unit vector normal to the plane of the loop. Here, the radius of the coil \( r = 0.1 \, \text{m} \), so the area is: \[ A = \pi (0.1)^2 = 0.01\pi \, \text{m}^2 \] The magnetic dipole moment is: \[ \vec{m} = 2 \times 0.01\pi \times \hat{n} = 0.02\pi \, \text{Am}^2 \] Since the current flows in the clockwise direction when viewed from above, the unit vector \( \hat{n} \) points in the \(-\hat{z}\) direction.
Thus, the magnetic dipole moment is \( 0.02\pi \, \text{Am}^2 \) in the \(-\hat{z}\) direction.
Two point charges M and N having charges +q and -q respectively are placed at a distance apart. Force acting between them is F. If 30% of charge of N is transferred to M, then the force between the charges becomes:
If the ratio of lengths, radii and Young's Moduli of steel and brass wires in the figure are $ a $, $ b $, and $ c $ respectively, then the corresponding ratio of increase in their lengths would be: