Step 1: Understanding intensity in Young's Double-Slit Experiment. The intensity at any point in an interference pattern is given by: \[ I = I_0 \left(1 + \cos \Delta \phi \right) \] where: - \( I_0 \) is the intensity of an individual wave, - \( \Delta \phi \) is the phase difference between the two waves. Step 2: Calculating intensity at \( P \) (where \( \Delta \phi = \frac{\pi}{3} \)). \[ I_P = I_0 \left(1 + \cos \frac{\pi}{3} \right) \] Since \( \cos \frac{\pi}{3} = \frac{1}{2} \), \[ I_P = I_0 \left(1 + \frac{1}{2} \right) = I_0 \times \frac{3}{2} = \frac{3I_0}{2} \]
Step 3: Calculating intensity at \( Q \) (where \( \Delta \phi = \frac{\pi}{2} \)). \[ I_Q = I_0 \left(1 + \cos \frac{\pi}{2} \right) \] Since \( \cos \frac{\pi}{2} = 0 \), \[ I_Q = I_0 \left(1 + 0 \right) = I_0 \]
Step 4: Finding the ratio \( I_P : I_Q \). \[ \frac{I_P}{I_Q} = \frac{\frac{3I_0}{2}}{I_0} = \frac{3}{2} \] Thus, the ratio of intensities: \[ I_P : I_Q = 3:2 \]
Final Answer: \[ \boxed{3:2} \]
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 \( \sqrt{5} = 2.23 \)) 