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Two different sound sources s(1) and s(2...

Two different sound sources `s_(1) and s_(2)` have frequencies ratio 1:2. Source s, is approaching towards an observer and `s_(2)` is receding from the same observer. Speeds of both `s_(1) and s_(2)` are the same and equal to v. speed of sound in air in 300 m/s. If no beats are heard by the observer the value of V is 1

A

125 m/s

B

100 m/s

C

75 m/s

D

50 m/s

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we will use the Doppler effect to find the speed \( V \) of the sound sources \( s_1 \) and \( s_2 \) given their frequency ratio and the conditions of the observer. ### Step-by-Step Solution: 1. **Identify the Frequencies**: Let the frequency of source \( s_1 \) be \( f \) and the frequency of source \( s_2 \) be \( 2f \) (since the ratio is 1:2). 2. **Doppler Effect for Approaching Source**: When source \( s_1 \) is approaching the observer, the observed frequency \( f' \) can be calculated using the Doppler effect formula: \[ f' = f \frac{v}{v - V} \] where \( v \) is the speed of sound in air (300 m/s) and \( V \) is the speed of source \( s_1 \). 3. **Doppler Effect for Receding Source**: For source \( s_2 \) which is receding from the observer, the observed frequency \( f'' \) is given by: \[ f'' = 2f \frac{v}{v + V} \] 4. **Condition for No Beats**: The condition for no beats to be heard by the observer is that the observed frequencies must be equal: \[ f' = f'' \] Substituting the expressions for \( f' \) and \( f'' \): \[ f \frac{v}{v - V} = 2f \frac{v}{v + V} \] 5. **Canceling \( f \)**: Since \( f \) is common on both sides, we can cancel it out (assuming \( f \neq 0 \)): \[ \frac{v}{v - V} = 2 \frac{v}{v + V} \] 6. **Cross Multiplying**: Cross multiplying gives: \[ v(v + V) = 2v(v - V) \] 7. **Expanding Both Sides**: Expanding both sides results in: \[ v^2 + vV = 2v^2 - 2vV \] 8. **Rearranging the Equation**: Rearranging gives: \[ vV + 2vV = 2v^2 - v^2 \] Simplifying: \[ 3vV = v^2 \] 9. **Solving for \( V \)**: Dividing both sides by \( v \) (assuming \( v \neq 0 \)): \[ 3V = v \] Thus, \[ V = \frac{v}{3} \] 10. **Substituting the Value of \( v \)**: Given \( v = 300 \, \text{m/s} \): \[ V = \frac{300}{3} = 100 \, \text{m/s} \] ### Final Answer: The value of \( V \) is \( 100 \, \text{m/s} \).
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