When the observer moves towards a stationary source with velocity '\(V_1\)', the apparent frequency of the emitted note is '\(F_1\)'. When the observer moves away from the source with velocity '\(V_1\)', the apparent frequency is '\(F_2\)'. If 'V' is the speed of sound in air and \(F_1/F_2 = 2\), then \(V/V_1 =\)