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Question: The difference between the apparent frequency of a source of sound as perceived by the observer duri...

The difference between the apparent frequency of a source of sound as perceived by the observer during its approach and recession is 2% of the frequency of the source. If the speed of the sound in air is 300ms1300m{{s}^{-1}}, the velocity of the source is:
A. 1.5ms11.5m{{s}^{-1}}
B. 12ms112m{{s}^{-1}}
C. 6ms16m{{s}^{-1}}
D. 3ms13m{{s}^{-1}}

Explanation

Solution

Hint: The difference in the apparent frequency and emitting frequency from the source is due to relative motion between source and observer. In this question the difference in frequency is noticed while source is approaching and receding. Therefore we apply the formula for change in frequency due to approach and due to recession and calculate the velocity of source.

Formula Used:
According to Doppler:
Apparent frequency observed by stationary observer while source is approaching towards observer is given by:
n1=n(vvvs){{n}_{1}}=n\left( \dfrac{v}{v-{{v}_{s}}} \right)
Apparent frequency observed by stationary observer while source is approaching towards observer is given by:
n2=n(vv+vs){{n}_{2}}=n\left( \dfrac{v}{v+{{v}_{s}}} \right)
Where:
nn is emitting frequency or original frequency
vv is the velocity of sound
vs{{v}_{s}} is the velocity of source

Complete step by step answer:

Change in frequency observed when the source is approaching and receding the stationary observer is known as beat.
Therefore,

Δn=n1n2\Delta n={{n}_{1}}-{{n}_{2}}
Apparent frequency due to approaching n1=n(vvvs){{n}_{1}}=n\left( \dfrac{v}{v-{{v}_{s}}} \right)
Apparent frequency due to recession n2=n(vv+vs){{n}_{2}}=n\left( \dfrac{v}{v+{{v}_{s}}} \right)
Δn=n(vvvs)n(vv+vs) Δn=nv[v+vsv+vsv2vs2] Δn=2nvvsv2(1vs2v2) v>>vs vs2v2<<1 Δn=2nvsv \begin{aligned} & \Delta n=n\left( \dfrac{v}{v-{{v}_{s}}} \right)-n\left( \dfrac{v}{v+{{v}_{s}}} \right) \\\ & \Delta n=nv\left[ \dfrac{v+{{v}_{s}}-v+{{v}_{s}}}{{{v}^{2}}-{{v}_{s}}^{2}} \right] \\\ & \Delta n=\dfrac{2nv{{v}_{s}}}{{{v}^{2}}\left( 1-\dfrac{{{v}_{s}}^{2}}{{{v}^{2}}} \right)} \\\ & v>>{{v}_{s}} \\\ & \therefore \dfrac{{{v}_{s}}^{2}}{{{v}^{2}}}<<1 \\\ & \Delta n=\dfrac{2n{{v}_{s}}}{v} \\\ \end{aligned}
It is given that Δn=2100n\Delta n=\dfrac{2}{100}n
Therefore:
2100n=2nvsv vs=v100 vs=300100=3ms1 \begin{aligned} & \dfrac{2}{100}n=\dfrac{2n{{v}_{s}}}{v} \\\ & {{v}_{s}}=\dfrac{v}{100} \\\ & {{v}_{s}}=\dfrac{300}{100}=3m{{s}^{-1}} \\\ \end{aligned}
Hence, the velocity of source is 3ms13m{{s}^{-1}}
Therefore, option D. is the correct answer

Note: Condition when Doppler Effect is not observed:
When both observer and source are at rest.
Both moving in the same direction with the same velocity.
Both moving parallel to each other with the same velocity.
Both moving perpendicular to each other.
When the medium alone is moving.
There is a limitation when Doppler Effect is not applicable is velocity of source, observer and medium must be less than the velocity of sound.