Step 1: The magnetic field outside a uniformly magnetized cylinder cannot generally be expressed as the gradient of a scalar function. This is because the magnetization generates a non-conservative magnetic field in the region outside the cylinder, which contradicts the option (A).
Step 2: The bound volume current density \( \mathbf{J}_b \) is related to the magnetization \( \mathbf{M} \) by: \[ \mathbf{J}_b = \nabla \times \mathbf{M}. \] Since the magnetization is uniform, its curl is zero, and thus, the bound volume current density is zero, making option (B) correct.
Step 3: The surface current density \( \mathbf{K}_b \) on the curved surface of the cylinder is given by: \[ \mathbf{K}_b = \hat{n} \times \mathbf{M}. \] Since the magnetization is uniform and along the axis of the cylinder, there is a non-zero surface current density on the curved surface, which makes option (C) correct.
Step 4: On the flat surfaces (top and bottom), the magnetization does not produce a current, as the magnetization is parallel to the cylinder's axis. Therefore, the surface current densities on the flat surfaces are zero, making option (D) incorrect.
| Column I | Column II |
(1)![]() | (P) Diamagnetic |
(2)![]() | (Q) Paramagnetic |
(3)![]() | (R) Ferromagnetic |
(4)![]() | (S) Antiferromagnetic |
The effective magnetic moment (in units of Bohr magneton) for the ground state of an isolated 4๐ ion with 6 unpaired electrons in the 4๐ shell according to Hundโs rules is (in integer) _____
The wire loop shown in the figure carries a steady current \( I \). Each straight section of the loop has length \( d \). A part of the loop lies in the \( xy \)-plane and the other part is tilted at \( 30^\circ \) with respect to the \( xz \)-plane. The magnitude of the magnetic dipole moment of the loop (in appropriate units) is:
