Doppler Effect
WAVES

172986 An observer and a source emitting sound of frequency $120 \mathrm{~Hz}$ are on the $\mathrm{X}$-axis. The observer is stationary while the source of sound is in motion given by the equation $x=3 \sin \omega t(x$ is in metres and $t$ is in seconds). If the difference between the maximum and minimum frequencies of the sound observed by the observers is $22 \mathrm{~Hz}$, then the value of $\omega$ is (speed of sound in air $=330 \mathrm{~ms}^{-1}$ )

1 $33 \mathrm{rad} \mathrm{ms}^{-1}$
2 $36 \mathrm{rad} \mathrm{ms}^{-1}$
3 $20 \mathrm{rad} \mathrm{ms}^{-1}$
4 $10 \mathrm{rad} \mathrm{ms}^{-1}$
WAVES

172987 A small source of sound vibrating at a frequency $500 \mathrm{~Hz}$ is rotated along a circle of radius $\frac{100}{\pi} \mathrm{cm}$ at a constant angular speed of 5 revolutions per second. The minimum and maximum frequency of the sound observed by a listener situation in the plane of the circle is (speed of sound is $332 \mathrm{~ms}^{-1}$ ).

1 $338.5 \mathrm{~Hz}, 612.5 \mathrm{~Hz}$
2 $485.4 \mathrm{~Hz}, 535.6 \mathrm{~Hz}$
3 $435.3 \mathrm{~Hz}, 565.6 \mathrm{~Hz}$
4 $485.4 \mathrm{~Hz}, 515.5 \mathrm{~Hz}$
WAVES

172991 When a train is approaching the stationary observer, the apparent frequency of the whistle of the train is $f_{1}$ and when the train is moving away from the observer, the apparent frequency in $f_{2}$. The frequency of the whistle noticed by the observer when he moves with the train is

1 $\frac{2 f_{1} f_{2}}{f_{1}+f_{2}}$
2 $\frac{f_{1} f_{2}}{f_{1}+f_{2}}$
3 $\frac{2 \mathrm{f}_{1} \mathrm{f}_{2}}{\mathrm{f}_{1}-\mathrm{f}_{2}}$
4 $\frac{\mathrm{f}_{1} \mathrm{f}_{2}}{\mathrm{f}_{1}-\mathrm{f}_{2}}$
WAVES

172992 A train moves towards a stationary observer with speed $34 \mathrm{~ms}^{-1}$. The train sounds a whistle and its frequency registered by the observer is $f_{1}$. If the speed of the train is reduced to $17 \mathrm{~ms}^{-1}$ the frequency registered is $f_{2}$. If the speed of sound is $340 \mathrm{~ms}^{-1}$, then the ratio $f_{1} / f_{2}$ is:

1 $18 / 19$
2 $1 / 2$
3 $19 / 18$
4 2
WAVES

172986 An observer and a source emitting sound of frequency $120 \mathrm{~Hz}$ are on the $\mathrm{X}$-axis. The observer is stationary while the source of sound is in motion given by the equation $x=3 \sin \omega t(x$ is in metres and $t$ is in seconds). If the difference between the maximum and minimum frequencies of the sound observed by the observers is $22 \mathrm{~Hz}$, then the value of $\omega$ is (speed of sound in air $=330 \mathrm{~ms}^{-1}$ )

1 $33 \mathrm{rad} \mathrm{ms}^{-1}$
2 $36 \mathrm{rad} \mathrm{ms}^{-1}$
3 $20 \mathrm{rad} \mathrm{ms}^{-1}$
4 $10 \mathrm{rad} \mathrm{ms}^{-1}$
WAVES

172987 A small source of sound vibrating at a frequency $500 \mathrm{~Hz}$ is rotated along a circle of radius $\frac{100}{\pi} \mathrm{cm}$ at a constant angular speed of 5 revolutions per second. The minimum and maximum frequency of the sound observed by a listener situation in the plane of the circle is (speed of sound is $332 \mathrm{~ms}^{-1}$ ).

1 $338.5 \mathrm{~Hz}, 612.5 \mathrm{~Hz}$
2 $485.4 \mathrm{~Hz}, 535.6 \mathrm{~Hz}$
3 $435.3 \mathrm{~Hz}, 565.6 \mathrm{~Hz}$
4 $485.4 \mathrm{~Hz}, 515.5 \mathrm{~Hz}$
WAVES

172991 When a train is approaching the stationary observer, the apparent frequency of the whistle of the train is $f_{1}$ and when the train is moving away from the observer, the apparent frequency in $f_{2}$. The frequency of the whistle noticed by the observer when he moves with the train is

1 $\frac{2 f_{1} f_{2}}{f_{1}+f_{2}}$
2 $\frac{f_{1} f_{2}}{f_{1}+f_{2}}$
3 $\frac{2 \mathrm{f}_{1} \mathrm{f}_{2}}{\mathrm{f}_{1}-\mathrm{f}_{2}}$
4 $\frac{\mathrm{f}_{1} \mathrm{f}_{2}}{\mathrm{f}_{1}-\mathrm{f}_{2}}$
WAVES

172992 A train moves towards a stationary observer with speed $34 \mathrm{~ms}^{-1}$. The train sounds a whistle and its frequency registered by the observer is $f_{1}$. If the speed of the train is reduced to $17 \mathrm{~ms}^{-1}$ the frequency registered is $f_{2}$. If the speed of sound is $340 \mathrm{~ms}^{-1}$, then the ratio $f_{1} / f_{2}$ is:

1 $18 / 19$
2 $1 / 2$
3 $19 / 18$
4 2
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WAVES

172986 An observer and a source emitting sound of frequency $120 \mathrm{~Hz}$ are on the $\mathrm{X}$-axis. The observer is stationary while the source of sound is in motion given by the equation $x=3 \sin \omega t(x$ is in metres and $t$ is in seconds). If the difference between the maximum and minimum frequencies of the sound observed by the observers is $22 \mathrm{~Hz}$, then the value of $\omega$ is (speed of sound in air $=330 \mathrm{~ms}^{-1}$ )

1 $33 \mathrm{rad} \mathrm{ms}^{-1}$
2 $36 \mathrm{rad} \mathrm{ms}^{-1}$
3 $20 \mathrm{rad} \mathrm{ms}^{-1}$
4 $10 \mathrm{rad} \mathrm{ms}^{-1}$
WAVES

172987 A small source of sound vibrating at a frequency $500 \mathrm{~Hz}$ is rotated along a circle of radius $\frac{100}{\pi} \mathrm{cm}$ at a constant angular speed of 5 revolutions per second. The minimum and maximum frequency of the sound observed by a listener situation in the plane of the circle is (speed of sound is $332 \mathrm{~ms}^{-1}$ ).

1 $338.5 \mathrm{~Hz}, 612.5 \mathrm{~Hz}$
2 $485.4 \mathrm{~Hz}, 535.6 \mathrm{~Hz}$
3 $435.3 \mathrm{~Hz}, 565.6 \mathrm{~Hz}$
4 $485.4 \mathrm{~Hz}, 515.5 \mathrm{~Hz}$
WAVES

172991 When a train is approaching the stationary observer, the apparent frequency of the whistle of the train is $f_{1}$ and when the train is moving away from the observer, the apparent frequency in $f_{2}$. The frequency of the whistle noticed by the observer when he moves with the train is

1 $\frac{2 f_{1} f_{2}}{f_{1}+f_{2}}$
2 $\frac{f_{1} f_{2}}{f_{1}+f_{2}}$
3 $\frac{2 \mathrm{f}_{1} \mathrm{f}_{2}}{\mathrm{f}_{1}-\mathrm{f}_{2}}$
4 $\frac{\mathrm{f}_{1} \mathrm{f}_{2}}{\mathrm{f}_{1}-\mathrm{f}_{2}}$
WAVES

172992 A train moves towards a stationary observer with speed $34 \mathrm{~ms}^{-1}$. The train sounds a whistle and its frequency registered by the observer is $f_{1}$. If the speed of the train is reduced to $17 \mathrm{~ms}^{-1}$ the frequency registered is $f_{2}$. If the speed of sound is $340 \mathrm{~ms}^{-1}$, then the ratio $f_{1} / f_{2}$ is:

1 $18 / 19$
2 $1 / 2$
3 $19 / 18$
4 2
WAVES

172986 An observer and a source emitting sound of frequency $120 \mathrm{~Hz}$ are on the $\mathrm{X}$-axis. The observer is stationary while the source of sound is in motion given by the equation $x=3 \sin \omega t(x$ is in metres and $t$ is in seconds). If the difference between the maximum and minimum frequencies of the sound observed by the observers is $22 \mathrm{~Hz}$, then the value of $\omega$ is (speed of sound in air $=330 \mathrm{~ms}^{-1}$ )

1 $33 \mathrm{rad} \mathrm{ms}^{-1}$
2 $36 \mathrm{rad} \mathrm{ms}^{-1}$
3 $20 \mathrm{rad} \mathrm{ms}^{-1}$
4 $10 \mathrm{rad} \mathrm{ms}^{-1}$
WAVES

172987 A small source of sound vibrating at a frequency $500 \mathrm{~Hz}$ is rotated along a circle of radius $\frac{100}{\pi} \mathrm{cm}$ at a constant angular speed of 5 revolutions per second. The minimum and maximum frequency of the sound observed by a listener situation in the plane of the circle is (speed of sound is $332 \mathrm{~ms}^{-1}$ ).

1 $338.5 \mathrm{~Hz}, 612.5 \mathrm{~Hz}$
2 $485.4 \mathrm{~Hz}, 535.6 \mathrm{~Hz}$
3 $435.3 \mathrm{~Hz}, 565.6 \mathrm{~Hz}$
4 $485.4 \mathrm{~Hz}, 515.5 \mathrm{~Hz}$
WAVES

172991 When a train is approaching the stationary observer, the apparent frequency of the whistle of the train is $f_{1}$ and when the train is moving away from the observer, the apparent frequency in $f_{2}$. The frequency of the whistle noticed by the observer when he moves with the train is

1 $\frac{2 f_{1} f_{2}}{f_{1}+f_{2}}$
2 $\frac{f_{1} f_{2}}{f_{1}+f_{2}}$
3 $\frac{2 \mathrm{f}_{1} \mathrm{f}_{2}}{\mathrm{f}_{1}-\mathrm{f}_{2}}$
4 $\frac{\mathrm{f}_{1} \mathrm{f}_{2}}{\mathrm{f}_{1}-\mathrm{f}_{2}}$
WAVES

172992 A train moves towards a stationary observer with speed $34 \mathrm{~ms}^{-1}$. The train sounds a whistle and its frequency registered by the observer is $f_{1}$. If the speed of the train is reduced to $17 \mathrm{~ms}^{-1}$ the frequency registered is $f_{2}$. If the speed of sound is $340 \mathrm{~ms}^{-1}$, then the ratio $f_{1} / f_{2}$ is:

1 $18 / 19$
2 $1 / 2$
3 $19 / 18$
4 2