According to de-Broglie hypothesis, the wavelength of the wave associated with electron while moving with velocity v is given by
λ = \(\frac{h}{mv}\) .........(i)
According to de-Broglie, stationary orbit is that orbit whose circumference is integral multiple of wavelength of wave associated with electron on that orbit.
If λ is the de-Broglie wavelength of electron while revolving in an orbit of radius r, then
2 πr = nλ
or λ = \(\frac{2\pi r}{n}\) ............(ii)
From (i) and (ii),
\(\frac{2\pi r }{n} = \frac{h}{mv}\)
or mvr = \( \frac{nh}{2\pi}\)
i.e. Total angular momentum = n \((\frac{h}{2\pi})\)
This is stated by Bohr about his stationary orbits.