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 ?

Given below are two statements. One is labelled as Assertion (A) and the other is labelled as Reason (R):
Assertion (A): An electron in a certain region of uniform magnetic field is moving with constant velocity in a straight line path.
Reason (R): The magnetic field in that region is along the direction of velocity of the electron.
In the light of the above statements, choose the correct answer from the options given below:
If the roots of $\sqrt{\frac{1 - y}{y}} + \sqrt{\frac{y}{1 - y}} = \frac{5}{2}$ are $\alpha$ and $\beta$ ($\beta > \alpha$) and the equation $(\alpha + \beta)x^4 - 25\alpha \beta x^2 + (\gamma + \beta - \alpha) = 0$ has real roots, then a possible value of $y$ is: