\( 340 \) Hz
Step 1: Relationship between path difference and phase difference
The phase difference \( \Delta \phi \) and path difference \( \Delta x \) of a wave are related by: \[ \Delta \phi = \frac{2\pi}{\lambda} \Delta x \] Given: \[ \Delta \phi = 1.8\pi, \quad \Delta x = 50 \text{ cm} = 0.50 \text{ m} \] Step 2: Solve for wavelength \( \lambda \)
Rearranging the equation: \[ \lambda = \frac{2\pi \times 0.50}{1.8\pi} \] \[ \lambda = \frac{1.0}{1.8} = 0.555 \text{ m} \] Step 3: Calculate frequency
The frequency of a wave is given by: \[ f = \frac{v}{\lambda} \] where \( v = 340 \) m/s is the speed of sound in air. \[ f = \frac{340}{0.555} \] \[ f \approx 612 \text{ Hz} \] Thus, the frequency of the sound wave is \( 612 \) Hz.
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 \( \sqrt{5} = 2.23 \)) 