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Problem
Problem
If
E
n
E_n
E
n
and
L
n
L_n
L
n
denote the total energy and the angular momentum of an electron in the *n*th orbit of Bohr atom, then a.
E
n
∝
L
n
E_n \propto L_n
E
n
∝
L
n
b.
E
n
∝
1
L
n
E_n \propto \frac{1}{L_n}
E
n
∝
L
n
1
c.
E
n
∝
L
n
2
E_n \propto L_n^2
E
n
∝
L
n
2
d.
E
n
∝
1
L
2
E_n \propto \frac{1}{L^2}
E
n
∝
L
2
1
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