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In a resonance tube with tuning fork of...

In a resonance tube with tuning fork of frequency `512 Hz`, first resonance occurs at water level equal to `30.3cm` and second resonance ocuurs at `63.7cm`. The maximum possible error in the speed of sound is

A

`5.12 cm//s`

B

`102.4 cm//s`

C

`204.8 cm//s`

D

`153.6 cm//s`

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To solve the problem, we need to determine the maximum possible error in the speed of sound based on the given resonance tube measurements. Here’s a step-by-step breakdown of the solution: ### Step 1: Understand the Resonance Condition In a resonance tube, the first resonance occurs when the length of the air column corresponds to a quarter of the wavelength (λ/4), and the second resonance occurs when the length corresponds to three-quarters of the wavelength (3λ/4). ### Step 2: Set Up the Equations Let: - \( L_1 = 30.3 \, \text{cm} \) (first resonance) - \( L_2 = 63.7 \, \text{cm} \) (second resonance) - \( e \) = end correction From the first resonance condition: \[ \frac{\lambda}{4} = L_1 + e \] (Equation 1) From the second resonance condition: \[ \frac{3\lambda}{4} = L_2 + e \] (Equation 2) ### Step 3: Subtract the Equations Subtract Equation 1 from Equation 2: \[ \frac{3\lambda}{4} - \frac{\lambda}{4} = (L_2 + e) - (L_1 + e) \] This simplifies to: \[ \frac{2\lambda}{4} = L_2 - L_1 \] Thus: \[ \frac{\lambda}{2} = L_2 - L_1 \] ### Step 4: Relate Wavelength to Speed of Sound The wavelength is related to the speed of sound (V) and frequency (f) by: \[ \lambda = \frac{V}{f} \] Substituting this into our equation gives: \[ \frac{V}{2f} = L_2 - L_1 \] ### Step 5: Solve for Speed of Sound Rearranging gives: \[ V = 2f(L_2 - L_1) \] ### Step 6: Calculate the Maximum Possible Error To find the maximum possible error in the speed of sound, we need to consider the errors in \( L_1 \) and \( L_2 \). The least count (error) in both measurements is \( 0.1 \, \text{cm} \). Let: - \( \Delta L_1 = 0.1 \, \text{cm} \) - \( \Delta L_2 = 0.1 \, \text{cm} \) The total error in the length difference \( L_2 - L_1 \) is: \[ \Delta(L_2 - L_1) = \Delta L_2 + \Delta L_1 = 0.1 + 0.1 = 0.2 \, \text{cm} \] ### Step 7: Substitute into the Error Formula The change in speed of sound \( \Delta V \) can be expressed as: \[ \Delta V = 2f \cdot \Delta(L_2 - L_1) \] Substituting the values: - \( f = 512 \, \text{Hz} \) - \( \Delta(L_2 - L_1) = 0.2 \, \text{cm} = 0.002 \, \text{m} \) Thus: \[ \Delta V = 2 \times 512 \times 0.002 = 2.048 \, \text{m/s} = 204.8 \, \text{cm/s} \] ### Final Answer The maximum possible error in the speed of sound is: \[ \Delta V = 204.8 \, \text{cm/s} \] ---

To solve the problem, we need to determine the maximum possible error in the speed of sound based on the given resonance tube measurements. Here’s a step-by-step breakdown of the solution: ### Step 1: Understand the Resonance Condition In a resonance tube, the first resonance occurs when the length of the air column corresponds to a quarter of the wavelength (λ/4), and the second resonance occurs when the length corresponds to three-quarters of the wavelength (3λ/4). ### Step 2: Set Up the Equations Let: - \( L_1 = 30.3 \, \text{cm} \) (first resonance) ...
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