The potential energy of the orbital electron in the ground state of hydrogen atoms is $-\mathrm{E}$. What is…
- $4 \mathrm{E}$
- $\frac{E}{4}$
- $\frac{E}{2}$
- $2 E$
Solution
$\frac{\mathrm{ze}^2}{4 \pi \varepsilon_0 \mathrm{r}^2}=\frac{\mathrm{mv}^2}{\mathrm{r}}$
$\therefore \mathrm{K}=\frac{\mathrm{mv}^2}{2}=\frac{1}{2}\left(\frac{\mathrm{ze}^2}{4 \pi \varepsilon_0 \mathrm{r}^2}\right)$
Thus, $\mathrm{K}=\frac{\mathrm{E}}{2}=\frac{\mathrm{U}}{2}$Asked in: MHT CET 2022 (08 Aug Shift 2)
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