$\mathrm{M}=\mathrm{N} \times \mathrm{I} \times \mathrm{n} \mathrm{R}^{2}$
$\mathrm{M}=\mathrm{N} \times \mathrm{I} \times \mathrm{N} \times \frac{\mathrm{L}^{2}}{4 \mathrm{n}^{2} \mathrm{N}^{2}}$
$\mathrm{L}=\mathrm{N} \times 2 \mathrm{nR}$
$\Rightarrow \mathrm{R}=\frac{\mathrm{L}}{2 \mathrm{nN}} \quad \mathrm{M} \times \frac{1}{\mathrm{N}}$
For $M_{\max } N=1$ and area of circle is maximum
$[A$ For $B>\frac{2}{3} \frac{p}{QR}$, the particle will re-enter region $1$
$[B]$ For $B=\frac{8}{13} \frac{\mathrm{p}}{QR}$, the particle will enter region $3$ through the point $P_2$ on $\mathrm{x}$-axis
$[C]$ When the particle re-enters region 1 through the longest possible path in region $2$ , the magnitude of the change in its linear momentum between point $P_1$ and the farthest point from $y$-axis is $p / \sqrt{2}$
$[D]$ For a fixed $B$, particles of same charge $Q$ and same velocity $v$, the distance between the point $P_1$ and the point of re-entry into region $1$ is inversely proportional to the mass of the particle
$(i)$ Electrons $(ii)$ Protons $(iii)$ $H{e^{2 + }}$ $(iv)$ Neutrons
The emission at the instant can be
