Obtain Gauss’s law from Coulomb’s law.
Coulombian force acting between charges $Q+q$ is,
$\mathrm{F}=\frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{\mathrm{Q} q}{r^{2}}$
$\frac{\mathrm{F}}{\mathrm{Q}}=\frac{q}{4 \pi \varepsilon_{0} \cdot r^{2}}$
$\text { But, } \frac{\mathrm{F}}{\mathrm{Q}}=\overrightarrow{\mathrm{E}}$
[Force acting on Q charge placed in electric field of $q$ means intensity of electric field E.]
$\therefore \mathrm{E}=\frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{q}{r^{2}}$
$\therefore \mathrm{E} \times 4 \pi r^{2}=\frac{q}{\varepsilon_{0}}$
$\therefore \int \mathrm{E} d s=\frac{q}{\varepsilon_{0}}, \text { where } 4 \pi r^{2}=d s$
As $\mathrm{E}$ and $d s$ are vectors,
$\int \overrightarrow{\mathrm{E}} \cdot \overrightarrow{d s}=\frac{q}{\varepsilon_{0}}$ This is Gauss's law.
Obtain the expression of electric field by ......
$(i)$ infinite size and with uniform charge distribution.
$(ii)$ thin spherical shell with uniform charge distribution at a point outside it.
$(iii)$ thin spherical shell with uniform charge distribution at a point inside it.
The electric field $\vec E = {E_0}y\hat j$ acts in the space in which a cylinder of radius $r$ and length $l$ is placed with its axis parallel to $y-$ axis. The charge inside the volume of cylinder is
Let there be a spherically symmetric charge distribution with charge density varying as $\rho (r)=\;\rho _0\left( {\frac{5}{4} - \frac{r}{R}} \right)$, upto $r = R$ ,and $\rho (r) = 0$ for $r > R$ , where $r$ is the distance from the origin. The electric field at a distance $r(r < R)$ from the origin is given by
Find the force experienced by the semicircular rod charged with a charge $q$, placed as shown in figure. Radius of the wire is $R$ and the line of charge with linear charge density $\lambda $ is passing through its centre and perpendicular to the plane of wire.
Two concentric conducting thin spherical shells of radii $a$ and $b\ (b > a)$ are given charges $Q$ and $ -2Q$ respectively. The electric field along a line passing through centre as a function of distance $(r)$ from centre is given by