



Step 1: Understanding the Electric Potential of a Non-Conducting Sphere For a uniformly charged non-conducting sphere: - Inside the sphere (\( r<R \)): The electric potential \( V \) at a distance \( r \) from the center is given by: \[ V = \frac{kQ}{2R} \left( 3 - \frac{r^2}{R^2} \right) \] This shows a parabolic decrease from the center to the surface. - Outside the sphere (\( r \geq R \)): The sphere behaves like a point charge, and the potential follows: \[ V = \frac{kQ}{r} \] which represents an inverse relationship with distance.
Step 2: Identifying the Correct Graph - Inside the sphere (\( r<R \)), \( V \) follows a quadratic relation. - Outside the sphere (\( r>R \)), \( V \) follows an inverse relation \( V \propto \frac{1}{r} \), which shows a smooth decrease. Among the given graphs, Graph D correctly represents this behavior: - A parabolic decrease inside the sphere. - A smooth inverse decrease outside the sphere.
The stopping potential (\(V_0\)) versus frequency (\(\nu\)) of a graph for the photoelectric effect in a metal is given. From the graph, the Planck's constant (\(h\)) is:

In the diagram shown below, both the strings AB and CD are made of the same material and have the same cross-section. The pulleys are light and frictionless. If the speed of the wave in string AB is \( v_1 \) and in CD is \( v_2 \), then the ratio \( \frac{v_1}{v_2} \) is:
