Question

A vibrating string of certain length $$\ell $$ under a tension $$T$$ resonates with a mode corresponding to the first overtone (third harmonic) of an air column of length $$75\,cm$$  inside a tube closed at one end. The string also generates 4 beats per second when excited along with a tuning fork of frequency $$n.$$ Now when the tension of the string is slightly increased the number of beats reduces 2 per second. Assuming the velocity of sound in air to be $$340\,m/s,$$  the frequency $$n$$ of the tuning fork in $$Hz$$  is

A. 344  
B. 336
C. 117.3
D. 109.3
Answer :   344
Solution :
The frequency $$\left( \nu \right)$$  produced by the air column is given by
$$\eqalign{ & \lambda \times \nu = \nu \cr & \Rightarrow \,\,\nu = \frac{\nu }{\lambda } \cr & {\text{Also, }}\frac{{3\lambda }}{4} = \ell = 75cm = 0.75m \cr & \therefore \,\,\lambda = \frac{{4 \times 0.75}}{3} \cr & \Rightarrow \,\nu = \frac{{340 \times 3}}{{4 \times 0.75}} \cr & = 340Hz \cr} $$
$$\therefore $$ The frequency of vibrating string = 340. Since this string produces 4 beats/sec with a tuning fork of frequency $$n$$ therefore $$n = 340 + 4$$   or $$n = 340 - 4.$$   With increase in tension, the frequency produced by string increases. As the beats/sec decreases therefore $$n = 340 + 4 = 344\,Hz.$$

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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