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: \[ \boxed{3:2} \]
A sub-atomic particle of mass \( 10^{-30} \) kg is moving with a velocity of \( 2.21 \times 10^6 \) m/s. Under the matter wave consideration, the particle will behave closely like (h = \( 6.63 \times 10^{-34} \) J.s)