The resultant intensity $I_R$ at a point in an interference pattern is given by \[I_R = I_1 + I_2 + 2 \sqrt{I_1 I_2} \cos \phi,\]where $I_1$ and $I_2$ are the intensities of the two sources, and $\phi$ is the phase difference between them. At point A, the phase difference is $\phi = \frac{\pi}{2}$, so \[I_A = I + 9I + 2 \sqrt{I \cdot 9I} \cos \frac{\pi}{2} = 10I.\]At point B, the phase difference is $\phi = \pi$, so \[I_B = I + 9I + 2 \sqrt{I \cdot 9I} \cos \pi = 10I - 6I = 4I.\]The difference in intensities is $I_A - I_B = 10I - 4I = \boxed{6I}$.
Final Answer: \( 6I \).
A transparent block A having refractive index $ \mu_2 = 1.25 $ is surrounded by another medium of refractive index $ \mu_1 = 1.0 $ as shown in figure. A light ray is incident on the flat face of the block with incident angle $ \theta $ as shown in figure. What is the maximum value of $ \theta $ for which light suffers total internal reflection at the top surface of the block ?
