$M=i A$
$M=\left(\frac{q}{T}\right) \times \pi r^{2}=\frac{q \pi r^{2}}{\left(\frac{2 \pi r}{v}\right)}=\frac{q v r}{2}$
$M=\frac{q v}{2} \times \frac{v m}{q B}$
$M =\frac{ mv ^{2}}{2 B }$
As we can see from the figure, direction of magnetic moment $(M)$ is opposite to magnetic field.
$\overrightarrow{ M }=-\frac{ mv ^{2}}{2 B } \hat{ B }$
$=-\frac{m v^{2}}{2 B^{2}} \vec{B}$
$(A)$ In the region $0 < r < R$, the magnetic field is non-zero.
$(B)$ In the region $R < r < 2 R$, the magnetic field is along the common axis.
$(C)$ In the region $R < r < 2 R$, the magnetic field is tangential to the circle of radius $r$, centered on the axis.
$(D)$ In the region $r > 2 R$, the magnetic field is non-zero.


Assertion $(A)$ : In an uniform magnetic field, speed and energy remains the same for a moving charged particle.
Reason $(R)$ : Moving charged particle experiences magnetic force perpendicular to its direction of motion.
Reason : $I_1 = I_2$ implies that the fields due to the current $I_1$ and $I_2$ will be balanced.