Question
With what potential an electron should be accelerated so that its de Broglie wavelength becomes equal to the wavelength of first line of lymen series for $He^+$ ion ?
$\Rightarrow \frac{\mathrm{h}}{\sqrt{2 \mathrm{meV}}}=\frac{1}{4 \mathrm{R}\left(\frac{3}{4}\right)}=\frac{1}{3 \mathrm{R}}$
$\frac{\mathrm{h}^{2}}{2 \mathrm{meV}}=\frac{1}{9 \mathrm{R}^{2}} \Rightarrow \mathrm{V}=\frac{9 \mathrm{R}^{2} \mathrm{h}^{2}}{2 \mathrm{me}}$
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| Column $I$ | Column $II$ |
| $(A)$ $u_x$ is doubled, $u_y$ is halved | $(p)$ $H$ will remain unchanged |
| $(B)$ $u_y$ is doubled $u_x$ is halved | $(q)$ $R$ will remain unchanged |
| $(C)$ $u_x$ and $u_y$ both are doubled | $(r)$ $R$ will become four times |
| $(D)$ Only $u_y$ is doubled | $(s)$ $H$ will become four times |