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A narrow pipe of length 2m is closed at ...

A narrow pipe of length 2m is closed at one end. The velocity of sound in air is 320 m/s. Neglecting end corrections , the air column in the pipe will resonate for sound of frequencies :

A

40Hz

B

80Hz

C

120Hz

D

160Hz

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To solve the problem, we need to determine the frequencies at which the air column in a closed pipe resonates. Here's a step-by-step solution: ### Step 1: Understand the fundamental frequency of a closed pipe For a pipe that is closed at one end, the fundamental frequency (first harmonic) can be calculated using the formula: \[ f_1 = \frac{v}{4L} \] where: - \(f_1\) is the fundamental frequency, - \(v\) is the velocity of sound in air, - \(L\) is the length of the pipe. ### Step 2: Substitute the values into the formula Given: - Length of the pipe, \(L = 2 \, \text{m}\) - Velocity of sound, \(v = 320 \, \text{m/s}\) Substituting these values into the formula: \[ f_1 = \frac{320 \, \text{m/s}}{4 \times 2 \, \text{m}} = \frac{320}{8} = 40 \, \text{Hz} \] ### Step 3: Determine the harmonic frequencies In a closed pipe, the resonant frequencies are given by the formula: \[ f_n = (2n - 1) f_1 \] where \(n\) is a positive integer (1, 2, 3, ...). ### Step 4: Calculate the first few harmonics - For \(n = 1\): \[ f_1 = (2 \times 1 - 1) \times 40 \, \text{Hz} = 1 \times 40 \, \text{Hz} = 40 \, \text{Hz} \] - For \(n = 2\): \[ f_2 = (2 \times 2 - 1) \times 40 \, \text{Hz} = 3 \times 40 \, \text{Hz} = 120 \, \text{Hz} \] - For \(n = 3\): \[ f_3 = (2 \times 3 - 1) \times 40 \, \text{Hz} = 5 \times 40 \, \text{Hz} = 200 \, \text{Hz} \] ### Step 5: List the resonant frequencies The resonant frequencies for the air column in the pipe are: - \(40 \, \text{Hz}\) - \(120 \, \text{Hz}\) - \(200 \, \text{Hz}\) ### Conclusion The air column in the pipe will resonate at frequencies of \(40 \, \text{Hz}\), \(120 \, \text{Hz}\), and \(200 \, \text{Hz}\). ---
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