Bohr’s quantization condition of angular momentum:
According to Bohr, electron can revolve only in certain discrete non-radiating orbits, called stationary orbits, for which total angular momentum of the revolving electron is an integral multiple of \(\frac{h}{2\pi}\)Where h is planck’s constant.
Thus, the angular momentum of the orbiting electron is quantized.
As, angular momentum of electron = mvr
∴ for any permitted (stationary) orbit
Where n = 1,2,3…… called as principal quantum number
Shortest wavelength, n2= ∞, n1 = 4
This wavelength belongs to infrared region of e.m. spectrum.