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To an observer, the pitch of a stationar...

To an observer, the pitch of a stationary source of sound appears to be reduced by 20%. If the speed of sound is 340m/s then speed and direction of the observer is

A

86 m/s towards the source

B

68 m/s towards the source

C

86 m/s away from the source

D

68 m/s away from the source

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem step by step, we will use the concept of the Doppler effect, which describes how the frequency of sound changes for an observer moving relative to a sound source. ### Step 1: Understand the Problem We know that the observer hears the frequency of the sound as reduced by 20%. This means the apparent frequency (\( f' \)) is 80% of the actual frequency (\( f \)). Therefore, we can express this relationship as: \[ f' = 0.8f \] ### Step 2: Identify the Doppler Effect Formula For a stationary source and a moving observer, the formula for the apparent frequency is given by: \[ f' = f \frac{v}{v + v_0} \] where: - \( f' \) = apparent frequency - \( f \) = actual frequency - \( v \) = speed of sound (340 m/s) - \( v_0 \) = speed of the observer (which we need to find) ### Step 3: Substitute the Known Values From the previous step, we know: \[ 0.8f = f \frac{340}{340 + v_0} \] We can cancel \( f \) from both sides (assuming \( f \neq 0 \)): \[ 0.8 = \frac{340}{340 + v_0} \] ### Step 4: Cross-Multiply to Solve for \( v_0 \) Cross-multiplying gives us: \[ 0.8(340 + v_0) = 340 \] Expanding this: \[ 272 + 0.8v_0 = 340 \] ### Step 5: Isolate \( v_0 \) Now, we isolate \( v_0 \): \[ 0.8v_0 = 340 - 272 \] \[ 0.8v_0 = 68 \] ### Step 6: Solve for \( v_0 \) Dividing both sides by 0.8: \[ v_0 = \frac{68}{0.8} = 85 \text{ m/s} \] ### Step 7: Determine the Direction Since the observer hears a lower frequency (the pitch is reduced), it confirms that the observer is moving away from the stationary source. ### Final Answer The speed of the observer is \( 85 \text{ m/s} \) moving away from the source. ---
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