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Q. A proton, a deuteron and an $\alpha$ - particle having the same kinetic energy are moving in circular trajectories in a constant magnetic field. If $r_{p^{\prime}} r_{d}$ and $r_{\alpha}$ denote respectively the radii of the trajectories of these particles, then

Solution:

$r=\frac{m v}{q B}=\frac{\sqrt{2 m K}}{q B} \propto \frac{\sqrt{m}}{q}$