Step 1: Apply Gauss's Law. Gauss's Law states that the net electric flux through any closed surface is proportional to the net electric charge enclosed by that surface (\( \Phi_E = \oint \vec{E} \cdot d\vec{A} = \frac{Q_{enc}}{\epsilon_0} \)).
Step 2: Consider a Gaussian surface inside the hollow conductor. For a hollow spherical conductor, any charge placed on it will reside entirely on its outer surface due to electrostatic repulsion. If we draw a spherical Gaussian surface at any radius \(r\) inside the hollow conductor, this surface encloses no charge (\(Q_{enc} = 0\)).
Step 3: Conclude the value of the electric field. Since \(Q_{enc} = 0\), Gauss's Law gives: \[ \oint \vec{E} \cdot d\vec{A} = 0 \] Due to the spherical symmetry, the electric field \(E\) must be constant in magnitude on the Gaussian surface and directed radially. Therefore, the integral becomes \( E \cdot (4\pi r^2) = 0 \). Since the area \(4\pi r^2\) is not zero, the electric field \(E\) must be zero everywhere inside the conductor.
Given below are two statements: one is labelled as Assertion A and the other is labelled as Reason R
Assertion A: Work done in moving a test charge between two points inside a uniformly charged spherical shell is zero, no matter which path is chosen.
Reason R: Electrostatic potential inside a uniformly charged spherical shell is constant and is same as that on the surface of the shell.
In the light of the above statements, choose the correct answer from the options given below
Two infinite identical charged sheets and a charged spherical body of charge density ' $\rho$ ' are arranged as shown in figure. Then the correct relation between the electrical fields at $\mathrm{A}, \mathrm{B}, \mathrm{C}$ and D points is:
