(Speed of sound $v = 340\, m/s$)
${n_a} = \left( {\frac{v}{{v - {v_S}}}} \right) \times n = \left( {\frac{{340}}{{340 - 20}}} \right) \times 1000 = 1063Hz$
When source is receding, the frequency heard
${n_r} = \left( {\frac{v}{{v + {v_S}}}} \right) \times n$=$\frac{{340}}{{340 + 20}} \times 1000 = 944$
$ \Rightarrow {n_a}:{n_r} = 9:8$
Short trick : $\frac{{{n_a}}}{{{n_r}}} = \frac{{v + {v_S}}}{{v - {v_S}}} = \frac{{340 + 20}}{{340 - 20}} = \frac{9}{8}.$
(image)
[$A$] The time $\mathrm{T}_{A 0}=\mathrm{T}_{\mathrm{OA}}$
[$B$] The velocities of the two pulses (Pulse $1$ and Pulse $2$) are the same at the midpoint of rope.
[$C$] The wavelength of Pulse $1$ becomes longer when it reaches point $A$.
[$D$] The velocity of any pulse along the rope is independent of its frequency and wavelength.
${y_1} = 10\,\sin \,200\pi t$,
${y_2} = 20\,\sin \,\left( {2000\pi t + \frac{\pi }{2}} \right)$
are superimposed at any point at a particular instant. The amplitude of the resultant wave is