In Young's double slit experiment, the intensity at any point on the screen is determined by the superposition of two wave amplitudes from the coherent sources. The relationship between the maximum intensity \(I_{\text{max}}\) and the minimum intensity \(I_{\text{min}}\) in terms of amplitude \(A_1\) and \(A_2\) is given by:
\(I_{\text{max}} = (A_1 + A_2)^2\)
\(I_{\text{min}} = (A_1 - A_2)^2\)
Given that the ratio of maximum and minimum intensities is 9:1:
\(\frac{I_{\text{max}}}{I_{\text{min}}} = \frac{(A_1 + A_2)^2}{(A_1 - A_2)^2} = 9\)
Taking the square root on both sides, we get:
\(\frac{A_1 + A_2}{A_1 - A_2} = 3\)
Cross-multiplying gives:
\(A_1 + A_2 = 3(A_1 - A_2)\)
Expanding and rearranging terms:
\(A_1 + A_2 = 3A_1 - 3A_2\)
\(A_2 + 3A_2 = 3A_1 - A_1\)
\(4A_2 = 2A_1\)
\(\frac{A_1}{A_2} = \frac{4}{2} = 2:1\)
Thus, the ratio of the amplitudes of coherent sources is 2:1.
In Young's double slit experiment, the intensity of the interference fringes depends on the amplitudes of the coherent sources.
The maximum intensity \( I_{\text{max}} \) and the minimum intensity \( I_{\text{min}} \) are related to the amplitudes \( A_1 \) and \( A_2 \) of the two waves as follows: \[ I_{\text{max}} = (A_1 + A_2)^2 \] \[ I_{\text{min}} = (A_1 - A_2)^2 \] The ratio of maximum and minimum intensities is given by: \[ \frac{I_{\text{max}}}{I_{\text{min}}} = \frac{(A_1 + A_2)^2}{(A_1 - A_2)^2} \] Given that the ratio of maximum and minimum intensities is 9:1, we have: \[ \frac{(A_1 + A_2)^2}{(A_1 - A_2)^2} = 9 \] Taking the square root of both sides: \[ \frac{A_1 + A_2}{A_1 - A_2} = 3 \] Solving for the ratio of the amplitudes: \[ A_1 + A_2 = 3(A_1 - A_2) \] Expanding and simplifying: \[ A_1 + A_2 = 3A_1 - 3A_2 \] \[ A_1 + A_2 - 3A_1 + 3A_2 = 0 \] \[ -2A_1 + 4A_2 = 0 \] \[ A_1 = 2A_2 \]
Thus, the ratio of the amplitudes is \( A_1 : A_2 = 2:1 \). Therefore, the correct answer is: \[ \text{(C) } 2:1 \]
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: