\( 2:3 \)
Step 1: Applying the Doppler effect formula
The observed frequency when the observer is moving away from the stationary source is given by: \[ f' = f \times \frac{v}{v + v_o} \] where: - \( f = 102 \) Hz (source frequency), - \( v \) is the speed of sound in air, - \( v_o = 0.1 v \) (observer’s speed moving away).
Step 2: Compute the observed frequencies
For observer 1 moving away: \[ f'_1 = 102 \times \frac{v}{v + 0.1v} \] \[ = 102 \times \frac{v}{1.1v} \] \[ = 102 \times \frac{1}{1.1} \] \[ \approx 92.7 \text{ Hz} \] For observer 2 moving in the opposite direction, the same calculation applies: \[ f'_2 = 102 \times \frac{v}{1.1v} = 92.7 \text{ Hz} \]
Step 3: Find the ratio of frequencies
\[ \frac{f'_1}{f'_2} = \frac{92.7}{92.7} = 1:1 \] Thus, the ratio of the frequencies of sound heard by the observers is \( 1:1 \).
Two loudspeakers (\(L_1\) and \(L_2\)) are placed with a separation of \(10 \, \text{m}\), as shown in the figure. Both speakers are fed with an audio input signal of the same frequency with constant volume. A voice recorder, initially at point \(A\), at equidistance to both loudspeakers, is moved by \(25 \, \text{m}\) along the line \(AB\) while monitoring the audio signal. The measured signal was found to undergo \(10\) cycles of minima and maxima during the movement. The frequency of the input signal is _____________ Hz.
(Speed of sound in air is \(324 \, \text{m/s}\) and \( \sqrt{5} = 2.23 \)) 