Two large thin conducting plates with a small gap in between are placed in a uniform electric field $E$ (perpendicular to the plates). The area of each plate is $A,$ and charges $+Q$ and $-Q$ are given to these plates as shown in figure. If $R, S,$ and $T$ are three points in space, then the

The figure shows a point charge of $0.5\times {10}^{-6} \mathrm{C}$ at the centre of a spherical cavity of radius $3 \mathrm{cm}$ of a piece of metal. The electric field at,

A right circular imaginary cone is shown in the figure. $A, B,$ and $C$ are the points in the plane containing the base of the cone, while $D$ is the point at the vertex of the cone. If ${\mathrm{\varphi }}_{\mathrm{A}}\text{,} {\mathrm{\varphi }}_{\mathrm{B}}\text{,} {\mathrm{\varphi }}_{\mathrm{C}}$ and ${\mathrm{\varphi }}_{\mathrm{D}}$ represent the flux through the curved surface of the cone when a point charge $Q$ is at points $A\text{,} B\text{,} C\text{,}$ and $D$ respectively, then

$A$, $B$ and $C$ are three large, parallel conducting plates, placed horizontally. $A$ and $C$ are rightly fixed and earthed (figure). $B$ is given some charge. Under electrostatic and gravitational forces, $B$ maybe

An insulating spherical shell of uniform surface charge density is cut into two parts and placed at a distance $d$ apart as shown in figure. ${\overrightarrow{E}}_P$ and ${\overrightarrow{E}}_Q$ denote the electric fields at $P$ and $Q,$ respectively. As $d$ (i.e., $PQ$)$\to \infty$

The figure shows, in cross-section, two Gaussian spheres and two Gaussian cubes that are centered on a positively charged particle. Rank greatest first, and indicate whether the magnitudes are uniform or variable along each surface.

The figure shows four Gaussian surfaces consisting of identical cylindrical midsections but different end caps. The surfaces are in a uniform electric field that is directed parallel to the central axis of each cylindrical midsection. The end caps have these shapes: $S_1$, convex hemispheres; $S_2$, concave hemispheres; $S_3$, cones; $S_4$, flat disks. Rank the surfaces according to $\left(\mathrm{a}\right)$ the net electric flux through them and $\left(\mathrm{b}\right)$ the electric flux through the top end caps, the greatest first.