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A resonance air column shows resonance w...

A resonance air column shows resonance with a tuning fork of frequency 256 Hz at column lengths 33.4 cmand 101.8 cm. find (i) end-correction and (ii) the speed of sound in air.

A

1. `300 ms^(-1)`

B

2. `250ms^(-1)`

C

3. `390ms^(-1)`

D

4. `350ms^(-1)`

Text Solution

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The correct Answer is:
To solve the problem, we will follow these steps: ### Step 1: Understand the Resonance Condition In a resonance air column, the lengths at which resonance occurs correspond to specific harmonics of the sound wave. For a tube closed at one end, the resonant lengths correspond to odd multiples of a quarter wavelength. ### Step 2: Calculate the Wavelength The difference in lengths at which resonance occurs corresponds to half the wavelength (\( \lambda/2 \)). Given the two lengths: - \( L_1 = 33.4 \, \text{cm} \) - \( L_2 = 101.8 \, \text{cm} \) The difference is: \[ \Delta L = L_2 - L_1 = 101.8 \, \text{cm} - 33.4 \, \text{cm} = 68.4 \, \text{cm} \] Since this difference corresponds to \( \lambda/2 \): \[ \frac{\lambda}{2} = 68.4 \, \text{cm} \implies \lambda = 2 \times 68.4 \, \text{cm} = 136.8 \, \text{cm} \] ### Step 3: Calculate the End Correction The length of the air column at resonance can be expressed as: \[ L_n = \frac{n\lambda}{4} + e \] where \( e \) is the end correction. For the first resonance (n=1): \[ L_1 = \frac{1 \times \lambda}{4} + e \] Substituting \( L_1 \) and \( \lambda \): \[ 33.4 \, \text{cm} = \frac{136.8 \, \text{cm}}{4} + e \] Calculating \( \frac{136.8}{4} \): \[ \frac{136.8}{4} = 34.2 \, \text{cm} \] Now substituting back: \[ 33.4 \, \text{cm} = 34.2 \, \text{cm} + e \implies e = 33.4 \, \text{cm} - 34.2 \, \text{cm} = -0.8 \, \text{cm} \] ### Step 4: Calculate the Speed of Sound The speed of sound \( v \) can be calculated using the formula: \[ v = f \cdot \lambda \] Given \( f = 256 \, \text{Hz} \) and converting \( \lambda \) to meters: \[ \lambda = 136.8 \, \text{cm} = 1.368 \, \text{m} \] Now substituting the values: \[ v = 256 \, \text{Hz} \times 1.368 \, \text{m} = 349.248 \, \text{m/s} \] Rounding this, we find: \[ v \approx 350 \, \text{m/s} \] ### Final Answers (i) End Correction, \( e = -0.8 \, \text{cm} \) (ii) Speed of Sound, \( v \approx 350 \, \text{m/s} \) ---

To solve the problem, we will follow these steps: ### Step 1: Understand the Resonance Condition In a resonance air column, the lengths at which resonance occurs correspond to specific harmonics of the sound wave. For a tube closed at one end, the resonant lengths correspond to odd multiples of a quarter wavelength. ### Step 2: Calculate the Wavelength The difference in lengths at which resonance occurs corresponds to half the wavelength (\( \lambda/2 \)). Given the two lengths: - \( L_1 = 33.4 \, \text{cm} \) ...
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