The correct option of this question will be (c).
Solution —
In this case, magnetic force provides necessary centripetal foree $i$.e.
$$q v B=\frac{m v^{2}}{r}$$
Radius of path, $r=\frac{m v}{B q}=\frac{\sqrt{2 m E}}{q B}$
$\therefore \quad r=\frac{\sqrt{2 m E}}{B q}=\frac{\sqrt{2 m_{1} E_{1}}}{B q}$
or $E_{1}=\frac{m E}{m_{1}}=\frac{\left(2 m_{1}\right)}{m_{1}} \times 50 \mathrm{keV} \quad\left[\because m=2 m_{1}\right]$ $=100 \mathrm{keV}$