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.
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:
The effective magnetic moment (in units of Bohr magneton) for the ground state of an isolated 4𝑓 ion with 6 unpaired electrons in the 4𝑓 shell according to Hund’s rules is (in integer) _____
The figure shows an opamp circuit with a 5.1 V Zener diode in the feedback loop. The opamp runs from \( \pm 15 \, {V} \) supplies. If a \( +1 \, {V} \) signal is applied at the input, the output voltage (rounded off to one decimal place) is:
A wheel of mass \( 4M \) and radius \( R \) is made of a thin uniform distribution of mass \( 3M \) at the rim and a point mass \( M \) at the center. The spokes of the wheel are massless. The center of mass of the wheel is connected to a horizontal massless rod of length \( 2R \), with one end fixed at \( O \), as shown in the figure. The wheel rolls without slipping on horizontal ground with angular speed \( \Omega \). If \( \vec{L} \) is the total angular momentum of the wheel about \( O \), then the magnitude \( \left| \frac{d\vec{L}}{dt} \right| = N(MR^2 \Omega^2) \). The value of \( N \) (in integer) is:
In the transistor circuit shown in the figure, \( V_{BE} = 0.7 \, {V} \) and \( \beta_{DC} = 400 \). The value of the base current in \( \mu A \) (rounded off to one decimal place) is: