Question

In the figure shown a source of sound of frequency $$510\,Hz$$  moves with constant velocity $${v_s} = 20\,m/s$$   in the direction shown. The wind is blowing at a constant velocity $${v_w} = 20\,m/s$$   towards an observer who is at rest at point $$B.$$ Corresponding to the sound emitted by the source at initial position $$A,$$ the frequency detected by the observer is equal to (speed of sound relative to air $$= 330\,m/s$$  )
Waves mcq question image

A. $$510\,Hz$$
B. $$500\,Hz$$
C. $$525\,Hz$$  
D. $$550\,Hz$$
Answer :   $$525\,Hz$$
Solution :
Apparent frequency
$$\eqalign{ & n' = n\frac{{\left( {u + {v_w}} \right)}}{{\left( {u + {v_w} - {v_s}\cos {{60}^ \circ }} \right)}} \cr & = \frac{{510\left( {330 + 20} \right)}}{{330 + 20 - 20\cos {{60}^ \circ }}} \cr & = 510 \times \frac{{350}}{{340}} = 525\,Hz \cr} $$

Releted MCQ Question on
Oscillation and Mechanical Waves >> Waves

Releted Question 1

A cylindrical tube open at both ends, has a fundamental frequency $$'f'$$ in air. The tube is dipped vertically in air. The tube is dipped vertically in water so that half of it is in water. The fundamental frequency of the air column in now

A. $$\frac{f}{2}$$
B. $$\frac{3\,f}{4}$$
C. $$f$$
D. $$2\,f$$
Releted Question 2

A wave represented by the equation $$y = a\cos \left( {k\,x - \omega t} \right)$$    is superposed with another wave to form a stationary wave such that point $$x = 0$$  is a node. The equation for the other wave is

A. $$a\sin \left( {k\,x + \omega t} \right)$$
B. $$ - a\cos \left( {k\,x - \omega t} \right)$$
C. $$ - a\cos \left( {k\,x + \omega t} \right)$$
D. $$ - a\sin \left( {k\,x - \omega t} \right)$$
Releted Question 3

An object of specific gravity $$\rho $$ is hung from a thin steel wire. The fundamental frequency for transverse standing waves in the wire is $$300\,Hz.$$  The object is immersed in water so that one half of its volume is submerged. The new fundamental frequency in $$Hz$$  is

A. $$300{\left( {\frac{{2\,\rho - 1}}{{2\,\rho }}} \right)^{\frac{1}{2}}}$$
B. $$300{\left( {\frac{{2\,\rho }}{{2\,\rho - 1}}} \right)^{\frac{1}{2}}}$$
C. $$300\left( {\frac{{2\,\rho }}{{2\,\rho - 1}}} \right)$$
D. $$300\left( {\frac{{2\,\rho - 1}}{{2\,\rho }}} \right)$$
Releted Question 4

A wave disturbance in a medium is described by $$y\left( {x,t} \right) = 0.02\cos \left( {50\,\pi t + \frac{\pi }{2}} \right)\cos \left( {10\,\pi x} \right)$$        where $$x$$ and $$y$$ are in metre and $$t$$ is in second

A. A node occurs at $$x = 0.15\,m$$
B. An antinode occurs at $$x = 0.3\,m$$
C. The speed wave is $$5\,m{s^{ - 1}}$$
D. The wave length is $$0.3\,m$$

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