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QJEEAdv18Ph1671: JEE Advanced 2018 Physics - Class 11 JEEAdv18Ph1671 Solution: In an experiment to measure the speed of sound by a resonating…

In an experiment to measure the speed of sound by a resonating air column, a tuning fork of frequency 500 Hz is used. The length of the air column is varied by changing the level of water in the resonance tube. Two successive resonances are heard at air columns of length 50.7 cm and 83.9 cm. Which of the following statements is (are) true?

Multiple Choice Options

  • A The speed of second determined from this experiment is 332ms−1
  • B The end correction in this experiment is 0.9 cm
  • C The wavelength of the sound wave is 66.4 cm
  • D The resonance at 50.7 cm corresponds to the fundamental harmonic

Step-by-Step Verified Solution

To determine which statements are true, we'll analyze the experiment step by step, using the theory of resonating air columns in a closed tube (closed at one end and open at the other).

Fundamentals of Resonance in a Closed Tube

For a tube closed at one end, the resonant lengths occur at:

Ln=(2n−14)λ+eL_n = \left( \frac{2n - 1}{4} \right) \lambda + e

where:

LnL_n is the length of the air column for the nthn^\text{th} resonance,

λ\lambda is the wavelength of the sound wave,

ee is the end correction,

n=1,2,3,…n = 1, 2, 3, \dots

Successive resonances (like those at L1L_1 and L2L_2 ) can be used to eliminate the end correction and find the wavelength.

Calculations

Step 1: Calculate the Wavelength ( λ\lambda )

Given:

First resonance length ( L1L_1 ) = 50.7 cm

Second resonance length ( L2L_2 ) = 83.9 cm

The difference between successive resonances in a closed tube is:

L2−L1=λ2L_2 - L_1 = \frac{\lambda}{2}

Solving for λ\lambda :

λ=2(L2−L1)=2(83.9 cm−50.7 cm)=2(33.2 cm)=66.4 cm\lambda = 2(L_2 - L_1) = 2(83.9\, \text{cm} - 50.7\, \text{cm}) = 2(33.2\, \text{cm}) = 66.4\, \text{cm}

Conclusion: The wavelength of the sound wave is 66.4 cm.

Option C is true.

Step 2: Calculate the Speed of Sound ( vv )

Using the relationship v=fλv = f\lambda :

Frequency ( ff ) = 500 Hz

Wavelength ( λ\lambda ) = 66.4 cm = 0.664 m

v=fλ=500 Hz×0.664 m=332 m/sv = f\lambda = 500\, \text{Hz} \times 0.664\, \text{m} = 332\, \text{m/s}

Conclusion: The speed of sound determined from the experiment is 332 m/s.

Option A is true.

Step 3: Calculate the End Correction ( ee )

Assuming the first resonance corresponds to the second harmonic ( n=2n = 2 ):

L1=(2n−14)λ+eL_1 = \left( \frac{2n - 1}{4} \right) \lambda + e

For n=2n = 2 :

L1=(34)λ+eL_1 = \left( \frac{3}{4} \right) \lambda + e

Solving for ee :

e=L1−(34)λ=50.7 cm−(34×66.4 cm)e = L_1 - \left( \frac{3}{4} \right) \lambda = 50.7\, \text{cm} - \left( \frac{3}{4} \times 66.4\, \text{cm} \right)

e=50.7 cm−49.8 cm=0.9 cme = 50.7\, \text{cm} - 49.8\, \text{cm} = 0.9\, \text{cm}

Conclusion: The end correction is 0.9 cm.

Option B is true.

Step 4: Determine if L1L_1 is the Fundamental Harmonic

Assuming L1L_1 corresponds to the fundamental harmonic ( n=1n = 1 ):

L1=(14)λ+eL_1 = \left( \frac{1}{4} \right) \lambda + e

e=L1−(14)λ=50.7 cm−16.6 cm=34.1 cme = L_1 - \left( \frac{1}{4} \right) \lambda = 50.7\, \text{cm} - 16.6\, \text{cm} = 34.1\, \text{cm}

An end correction of 34.1 cm is unreasonably large for typical experiments, indicating that L1L_1 does not correspond to the fundamental harmonic.

Conclusion: The resonance at 50.7 cm does not correspond to the fundamental harmonic.

Option D is false.

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