Question

What is the effect of humidity on sound waves when humidity increases?

A. Speed of sound waves increases  
B. Speed of sound waves decreases
C. Speed of sound waves remains same
D. Speed of sound waves becomes zero
Answer :   Speed of sound waves increases
Solution :
The presence of water vapours in air changes its density. That is why the velocity of sound changes with humidity of air.
Suppose,
$${\rho _m} = $$ density of moist air
$${\rho _d} = $$ density of dry air
$${v_m} = $$ velocity of sound in moist air
$${v_d} = $$ velocity of sound in dry air
Assuming that effect of humidity on $$\gamma $$ is negligible.
As velocity of wave in a medium is given by
\[\therefore {v_m} = \sqrt {\frac{{\gamma p}}{{{\rho _m}}}} \,\,\left[ {\begin{array}{*{20}{c}} {\gamma = {\text{elasticity of medium}}} \\ {{\rho _m} = {\text{density of medium}}} \\ {p = {\text{pressure of sound waves}}} \end{array}} \right]\]
$$\eqalign{ & {\text{and}}\,\,{v_d} = \sqrt {\frac{{\gamma p}}{{{\rho _d}}}} \cr & {\text{Dividing, we get }}\frac{{{v_m}}}{{{v_d}}} = \sqrt {\frac{{{\rho _d}}}{{{\rho _m}}}} \cr} $$
The presence of water vapours reduces the density of air.
$${\text{i}}{\text{.e}}{\text{.}}\,{\rho _m} < {\rho _d}$$
Hence, velocity of sound in moist air is greater, then the velocity of sound in dry air.

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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Waves


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