When the observer moves towards a stationary source with velocity \( V_o \), the apparent frequency of emitted note is \( F_1 \). When the observer moves away from the source with velocity \( V_o \), the apparent frequency is \( F_2 \). If \( V \) is the velocity of sound in air and \( \frac{F_1}{F_2} = 2 \), then \( \frac{V}{V_o} \) is equal to