Question

A sonometer wire when vibrated in full length has frequency $$n.$$ Now, it is divided by the help of bridges into a number of segments of lengths $${l_1},{l_2},{l_3},\,....$$   When vibrated these segments have frequencies $${n_1},{n_2},{n_3},\,....$$   Then, the correct relation is

A. $$n = {n_1} + {n_2} + {n_3} + ....$$
B. $${n^2} = n_1^2 + n_2^2 + n_3^2 + \,....$$
C. $$\frac{1}{n} = \frac{1}{{{n_1}}} + \frac{1}{{{n_2}}} + \frac{1}{{{n_3}}} + \,.....$$  
D. $$\frac{1}{{\sqrt n }} = \frac{1}{{\sqrt {{n_1}} }} + \frac{1}{{\sqrt {{n_2}} }} + \frac{1}{{\sqrt {{n_3}} }} + \,.....$$
Answer :   $$\frac{1}{n} = \frac{1}{{{n_1}}} + \frac{1}{{{n_2}}} + \frac{1}{{{n_3}}} + \,.....$$
Solution :
From law of length, the frequency of vibrating string is inversely proportional to its length,
\[{\text{i}}{\text{.e}}{\text{.}}\,\,n \propto \frac{1}{l}\,\,\left[ {\begin{array}{*{20}{c}} {n = {\text{frequency of string}}} \\ {l = {\text{length of string}}} \end{array}} \right]\]
$$\eqalign{ & {\text{or}}\,\,nl = {\text{constant}}\left( {{\text{say}}\,k} \right) \cr & {\text{or}}\,\,l = \frac{k}{n} \cr} $$
The segments of string of length $${l_1},{l_2},{l_3},\,....$$   have frequencies $${n_1},{n_2},{n_3},\,....$$
Total length of string is $$l.$$
$$\eqalign{ & {\text{So,}}\,\,l = {l_1} + {l_2} + {l_3} + \,.... \cr & \therefore \frac{k}{n} = \frac{k}{{{n_1}}} + \frac{k}{{{n_2}}} + \frac{k}{{{n_3}}} + \,.... \cr & {\text{or}}\,\,\frac{1}{n} = \frac{1}{{{n_1}}} + \frac{1}{{{n_2}}} + \frac{1}{{{n_3}}} + \,.... \cr} $$

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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Waves


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