When the listener moves towards stationary source with velocity ' \mathrm{V}_1 ', the apparent frequency of emitted note is ' F_1 '. When observer moves away from the source with velocity ' \mathrm{V}_1 ', apparent frequency is ' F_2 '. If V is the velocity of sound in air and \frac{F_1}{F_2}=2 then \frac{V}{V_1} is