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The tension, length, diameter and densit...

The tension, length, diameter and density of a string B are double than that of another string A. Which of the following overtones of B is same as the fundamental frequency of A?

A

(a)1st

B

(b)2nd

C

(c)3rd

D

(d)4th

Text Solution

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The correct Answer is:
To solve the problem, we need to determine which overtone of string B corresponds to the fundamental frequency of string A, given that the tension, length, diameter, and density of string B are all double those of string A. ### Step-by-Step Solution: 1. **Understanding the Frequency Formula**: The frequency \( f \) of a vibrating string can be expressed as: \[ f = \frac{V}{\lambda} \] where \( V \) is the wave speed and \( \lambda \) is the wavelength. 2. **Wave Speed Formula**: The wave speed \( V \) on a string is given by: \[ V = \sqrt{\frac{T}{\mu}} \] where \( T \) is the tension in the string and \( \mu \) is the linear mass density (mass per unit length). 3. **Linear Mass Density**: The linear mass density \( \mu \) can be calculated as: \[ \mu = \frac{m}{L} \] where \( m \) is the mass of the string and \( L \) is its length. The mass can also be expressed in terms of volume and density: \[ m = \text{density} \times \text{volume} = \text{density} \times (\text{cross-sectional area} \times L) \] 4. **Calculating Frequencies**: - For string A: \[ f_A = \sqrt{\frac{T_A}{\mu_A}} \cdot \frac{1}{\lambda_A} \] The wavelength for the fundamental frequency (first harmonic, \( n=1 \)) is: \[ \lambda_A = 2L_A \] Thus: \[ f_A = \sqrt{\frac{T_A}{\mu_A}} \cdot \frac{1}{2L_A} \] - For string B: Given that tension, length, diameter, and density of string B are double those of A: \[ T_B = 2T_A, \quad L_B = 2L_A, \quad \mu_B = \frac{2 \cdot \text{density}_A \cdot \text{cross-sectional area}}{2L_A} = \frac{2\mu_A}{2} = \mu_A \] The wavelength for the fundamental frequency of string B is: \[ \lambda_B = 2L_B = 4L_A \] Thus: \[ f_B = \sqrt{\frac{T_B}{\mu_B}} \cdot \frac{1}{\lambda_B} = \sqrt{\frac{2T_A}{\mu_A}} \cdot \frac{1}{4L_A} \] 5. **Equating Frequencies**: We need to find \( n \) such that: \[ f_B = f_A \] From the expressions derived, we can equate: \[ \sqrt{\frac{2T_A}{\mu_A}} \cdot \frac{1}{4L_A} = \sqrt{\frac{T_A}{\mu_A}} \cdot \frac{1}{2L_A} \] Simplifying this gives: \[ \frac{1}{4} \sqrt{2} = \frac{1}{2} \] This implies that \( n = 2 \) corresponds to the second harmonic of string B. 6. **Finding the Overtone**: The overtone is defined as \( n - 1 \). Therefore, if the second harmonic corresponds to \( n = 2 \), the first overtone is: \[ \text{First overtone} = n - 1 = 2 - 1 = 1 \] ### Final Answer: The first overtone of string B is the same as the fundamental frequency of string A.

To solve the problem, we need to determine which overtone of string B corresponds to the fundamental frequency of string A, given that the tension, length, diameter, and density of string B are all double those of string A. ### Step-by-Step Solution: 1. **Understanding the Frequency Formula**: The frequency \( f \) of a vibrating string can be expressed as: \[ f = \frac{V}{\lambda} ...
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