To solve the problem, we need to determine the magnetic force on the arm $AC$ when the given current-carrying loop is subjected to a uniform magnetic field acting along $AB$.
The setup describes a right angle isosceles triangle, implying that the sides $AB$ and $AC$ are equal, and side $BC$ is the hypotenuse.
Key physics concepts involved in this problem include:
Since the magnetic field is along $AB$, there is no force on $AB$ (because the angle between $L$ and $B$ is zero and $\sin 0 = 0$). However, forces will act on $AC$ and $BC$.
Force on Arm $BC$: The problem states that the force on $BC$ is $\vec{F}$.
Force on Arm $AC$: As $BC$ and $AC$ are the arms of the triangle, they are perpendicular to each other. By symmetry and using the equilibrium condition (since a current loop in a uniform magnetic field will attempt to align itself such that the net force is zero), the force on $AC$ will be equal in magnitude and opposite in direction to the force on $BC$.
Thus, the force on $AC$ is -\vec{F}.
The correct answer is: -\vec{F}.
The magnetic moment is associated with its spin angular momentum and orbital angular momentum. Spin only magnetic moment value of Cr^{3+ ion (Atomic no. : Cr = 24) is: