The magnitude of total energy and angular momentum of an electron in the $n^{th}$ orbit of a Bohr atom is denoted by $E_{n}$ and $L_{n}$ respectively. Then

  • A
    $E_{n} \propto L_{n}$
  • B
    $E_{n} \propto L_{n}^{3}$
  • C
    $E_{n} \propto \frac{1}{L_{n}^{2}}$
  • D
    $E_{n} \propto \frac{1}{L_{n}}$

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