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A train moves towards a stationary observer with speed `34 m//s`. The train sounds a whistle and its frequency registered by the observer is `f_(1)`. If the train's speed is reduced to `17 m//s`, the frequency registered is `f_(2)`. If the speed of sound of `340 m//s`, then the ratio `f_(1)//f_(2)`is

A

`18//19`

B

`1//2`

C

`2`

D

`19//18`

Text Solution

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The correct Answer is:
To solve the problem, we will use the Doppler effect formula for sound waves. The formula for the frequency observed when the source is moving towards a stationary observer is given by: \[ f' = f \frac{c}{c - v_s} \] Where: - \(f'\) is the frequency observed, - \(f\) is the frequency of the source, - \(c\) is the speed of sound, - \(v_s\) is the speed of the source (train). ### Step 1: Calculate \(f_1\) when the train moves at 34 m/s Given: - Speed of sound, \(c = 340 \, m/s\) - Speed of the train, \(v_s = 34 \, m/s\) Using the formula for \(f_1\): \[ f_1 = f \frac{c}{c - v_s} = f \frac{340}{340 - 34} = f \frac{340}{306} \] This simplifies to: \[ f_1 = f \frac{340}{306} = \frac{170}{153} f \quad \text{(by dividing numerator and denominator by 2)} \] ### Step 2: Calculate \(f_2\) when the train moves at 17 m/s Now, when the speed of the train is reduced to \(v_s = 17 \, m/s\): \[ f_2 = f \frac{c}{c - v_s} = f \frac{340}{340 - 17} = f \frac{340}{323} \] ### Step 3: Calculate the ratio \(\frac{f_1}{f_2}\) Now we can find the ratio of \(f_1\) to \(f_2\): \[ \frac{f_1}{f_2} = \frac{\frac{170}{153} f}{\frac{340}{323} f} \] The \(f\) cancels out: \[ \frac{f_1}{f_2} = \frac{170}{153} \cdot \frac{323}{340} \] ### Step 4: Simplify the ratio Calculating the ratio: \[ \frac{f_1}{f_2} = \frac{170 \times 323}{153 \times 340} \] Calculating the values: - \(170 \times 323 = 54910\) - \(153 \times 340 = 52020\) Thus, \[ \frac{f_1}{f_2} = \frac{54910}{52020} \] This simplifies to approximately: \[ \frac{f_1}{f_2} \approx \frac{19}{18} \] ### Final Answer The ratio \(\frac{f_1}{f_2}\) is: \[ \frac{f_1}{f_2} = \frac{19}{18} \] ---

To solve the problem, we will use the Doppler effect formula for sound waves. The formula for the frequency observed when the source is moving towards a stationary observer is given by: \[ f' = f \frac{c}{c - v_s} \] Where: - \(f'\) is the frequency observed, ...
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