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The magnitude of total energy and angular momentum of an electron in the $\mathrm{n}^{\mathrm{th}}$ orbit of a Bohr atom is denoted by $E_{n}$ and $L_{n}$ respectively. Then
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$\mathrm{E}_{\mathrm{n}} \propto \frac{1}{\mathrm{~L}_{\mathrm{n}}^{2}}$
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