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: \( 6I \).
\(XPQY\) is a vertical smooth long loop having a total resistance \(R\), where \(PX\) is parallel to \(QY\) and the separation between them is \(l\). A constant magnetic field \(B\) perpendicular to the plane of the loop exists in the entire space. A rod \(CD\) of length \(L\,(L>l)\) and mass \(m\) is made to slide down from rest under gravity as shown. The terminal speed acquired by the rod is _______ m/s. 
A biconvex lens is formed by using two plano-convex lenses as shown in the figure. The refractive index and radius of curvature of surfaces are also mentioned. When an object is placed on the left side of the lens at a distance of \(30\,\text{cm}\), the magnification of the image will be: 
