A) half integral multiple of \[\frac{h}{2\pi }\]
B) integral multiple of h
C) integral multiple of \[\frac{h}{2\pi }\]
D) half integral multiple of h
Correct Answer: C
Solution :
For an electron to remain orbiting around the nucleus, the .angular momentum (L) should be an integral multiple of \[h/2\pi \]. ie, \[mvr=\frac{nh}{2\pi }\] where n = principle quantum number of electron, and h = Planck's constant
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