When the observer moves towards a 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 \(\mathrm{V}_1\), the apparent frequency is \(\mathrm{F}_2\). If V is the velocity of sound in air and \(F_1 / F_2=2\) then \(V / V_1\) is equal to