When an observer moves towards a stationary source with velocity '\(V_1\)', the apparent frequency of emitted note is '\(F_1\)'. When observer moves away from stationary source with velocity '\(V_1\)' the apparent frequency is '\(F_2\)'. If '\(v\)' is velocity of sound in air and \(\frac{F_1}{F_2} = 2\), then \(\frac{v}{V_1}\) is equal to
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Shortcut: If $F_1/F_2 = n$, then $v/V_1 = (n+1)/(n-1)$. Here $(2+1)/(2-1) = 3$.