MHT CET · Physics · Waves and Sound
A cylindrical tube open at both ends has fundamental frequency \(f\) in air. When the tube is dipped vertically in water so that one-third part of the tube is in water, the fundamental frequency of air column becomes (neglect end correction)
- A \(\frac{f}{2}\)
- B \(\frac{3 f}{2}\)
- C \(\frac{f}{4}\)
- D \(\frac{3 f}{4}\)
Answer & Solution
Correct Answer
(B) \(\frac{3 f}{2}\)
Step-by-step Solution
Detailed explanation
We know. Frequency is ratio of velocity of sound and wavelength:
\(f=\frac{v}{\lambda}\)
For tube of length , in fundamental mode wavelength is given by \(\frac{\lambda}{2}=L\)
\(\frac{\lambda}{2}=L\).
\(\therefore f=\frac{v}{2 L}\)
Now, if tube is dipped one third, then for fundamental mode in air column has:
\(\begin{aligned} & \frac{\lambda^{\prime}}{2}=\left(\frac{2}{3} L\right) \\ & \therefore f^{\prime}=\frac{3 v}{4 L}=\frac{3}{2} f\end{aligned}\)
\(f=\frac{v}{\lambda}\)
For tube of length , in fundamental mode wavelength is given by \(\frac{\lambda}{2}=L\)
\(\frac{\lambda}{2}=L\).
\(\therefore f=\frac{v}{2 L}\)
Now, if tube is dipped one third, then for fundamental mode in air column has:
\(\begin{aligned} & \frac{\lambda^{\prime}}{2}=\left(\frac{2}{3} L\right) \\ & \therefore f^{\prime}=\frac{3 v}{4 L}=\frac{3}{2} f\end{aligned}\)
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