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A tuning fork of frequency n is held nea...

A tuning fork of frequency n is held near the open end of tube, the tube is adjusted until resonance occurs. If the two shortest lengths to produce resonance are `L_1 and L_2` , then the speed of the sound is

A

`n(L_2-L_1)`

B

`(n(L_2-L_1))/2`

C

`4n(L_2-L_1)`

D

`2n(L_2-L_1)`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to find the speed of sound in a tube when resonance occurs at two different lengths, \( L_1 \) and \( L_2 \). Here’s a step-by-step solution: ### Step 1: Understanding the Resonance in the Tube When a tuning fork of frequency \( n \) is held near the open end of a tube, resonance occurs at specific lengths of the tube. For a tube that is open at one end and closed at the other, the lengths at which resonance occurs can be described by the formula for the wavelengths of the sound. ### Step 2: Wavelength and Length Relationship For a tube that is open at one end and closed at the other, the relationship between the length of the tube \( L \) and the wavelength \( \lambda \) of the sound wave is given by: \[ L = \frac{(2n - 1) \lambda}{4} \] where \( n \) is a positive integer (1, 2, 3, ...). ### Step 3: Expressing Wavelength in Terms of Lengths For the two shortest lengths \( L_1 \) and \( L_2 \) that produce resonance, we can write: - For \( L_1 \) (when \( n = 1 \)): \[ L_1 = \frac{(2 \cdot 1 - 1) \lambda}{4} = \frac{\lambda}{4} \] - For \( L_2 \) (when \( n = 2 \)): \[ L_2 = \frac{(2 \cdot 2 - 1) \lambda}{4} = \frac{3\lambda}{4} \] ### Step 4: Finding the Difference in Lengths Now, we find the difference between the two lengths: \[ L_2 - L_1 = \frac{3\lambda}{4} - \frac{\lambda}{4} = \frac{2\lambda}{4} = \frac{\lambda}{2} \] ### Step 5: Relating Wavelength to Speed of Sound The speed of sound \( v \) is related to the wavelength \( \lambda \) and frequency \( n \) by the equation: \[ v = n \lambda \] ### Step 6: Substituting Wavelength in Terms of Lengths From the previous steps, we have: \[ \lambda = 2(L_2 - L_1) \] Substituting this into the speed of sound equation: \[ v = n \cdot 2(L_2 - L_1) \] ### Step 7: Final Expression for Speed of Sound Thus, we can express the speed of sound as: \[ v = 2n(L_2 - L_1) \] ### Conclusion The speed of sound in the tube is given by: \[ v = 2n(L_2 - L_1) \]
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