When the electric flux associated with closed surface becomes positive, zero or negative ?
If electric flux associated with area $\overrightarrow{\mathrm{S}}$ due to electric field $E$ is $\phi$, then
$\phi=\overrightarrow{\mathrm{E}} \cdot \overrightarrow{\mathrm{S}}$ $\therefore \phi=\mathrm{EScos} \theta$ $\text { where } \theta \text { is angle between } \overrightarrow{\mathrm{E}} \text { and } \overrightarrow{\mathrm{S}}$ $\text { (i) } \quad \text { If } \overrightarrow{\mathrm{S}} \perp \overrightarrow{\mathrm{E}} \text { means surface is parallel to } \overrightarrow{\mathrm{E}} \text { then, }\theta=90^{\circ}$ $\therefore\text { From equation (1), }$ $\phi=\text { EScos0 }^{\circ}=0$ $\therefore\text{ Flux associated with surface is zero.}$
$(ii)$ If $\theta<90^{\circ}$, then $\cos \theta>0$ (positive) hence flux is positive.
$(iii)$ If $\theta>90^{\circ}$, then $\cos \theta<0$ (negative) hence flux is negative.
All three are shown in figure $(a)$, $(b)$ and $(c) $ respectively.
Obtain Gauss’s law from the flux associated with a sphere of radius $\mathrm{'r'}$ and charge $\mathrm{'q'}$ at centre.
If a charge $q$ is placed at the centre of a closed hemispherical non-conducting surface, the total flux passing through the flat surface would be
A positive charge $q$ is kept at the center of a thick shell of inner radius $R_1$ and outer radius $R_2$ which is made up of conducting material. If $\phi_1$ is flux through closed gaussian surface $S_1$ whose radius is just less than $R_1$ and $\phi_2$ is flux through closed gaussian surface $S_2$ whose radius is just greater than $R_1$ then:-
The figure shows two situations in which a Gaussian cube sits in an electric field. The arrows and values indicate the directions and magnitudes (in $N-m^2/C$) of the electric fields. What is the net charge (in the two situations) inside the cube?
Five charges $+q,+5 q,-2 q,+3 q$ and $-4 q$ are situated as shown in the figure.
The electric flux due to this configuration through the surface $S$ is