1. Magnetic Potential Energy: The magnetic potential energy (U) of a magnetic dipole (magnetic moment $\vec{m}$) in a magnetic field $\vec{B}$ is given by:
\[ U = -\vec{m} \cdot \vec{B} = -mB \cos\theta \]
where $\theta$ is the angle between the magnetic moment vector and the magnetic field vector.
2. Perpendicular Orientation ($\theta = 90^\circ$): When the magnetic bar is placed perpendicular to the magnetic field, the angle $\theta$ is $90^\circ$. Therefore, $\cos\theta = \cos(90^\circ) = 0$.
\[ U = -mB(0) = 0 \]
3. Conclusion: The magnetic potential energy is zero when the magnetic moment is perpendicular to the magnetic field.
A current-carrying coil is placed in an external uniform magnetic field. The coil is free to turn in the magnetic field. What is the net force acting on the coil? Obtain the orientation of the coil in stable equilibrium. Show that in this orientation the flux of the total field (field produced by the loop + external field) through the coil is maximum.
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The output (Y) of the given logic implementation is similar to the output of an/a …………. gate.