Answer:
Option A
Explanation:
When the observer is moving towards the source and source is stationary , then the apparent frequency is given as,
$n'=n\left(\frac{v+v_{0}}{v}\right)$ ..........(i)
When the observer is moving away from the source and the source is stationary , then the apparent frequency is given as,
$n''=-n\left(\frac{v-v_{0}}{v}\right)$ .......(ii)
From Eqs .(i) and (ii) , we get
$n'- n''=\frac{n}{v}(v'+v_{0}-v+v_{0})$
= $\frac {2nv_{0}}{v}$