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.
Two infinitely long parallel wires having linear charge densities ${\lambda _1}$ and ${\lambda _2}$ respectively are placed at a distance of $R$ metres. The force per unit length on either wire will be $\left( {K = \frac{1}{{4\pi {\varepsilon _0}}}} \right)$
Explain by graph how the electric field by thin spherical shell depends on the distance of point from centre.
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
Consider an atom with atomic number $Z$ as consisting of a positive point charge at the centre and surrounded by a distribution of negative electricity uniformly distributed within a sphere of radius $R$. The electric field at a point inside the atom at a distance $r$ from the centre is
A spherically symmetric charge distribution is considered with charge density varying as
$\rho(r)=\left\{\begin{array}{ll}\rho_{0}\left(\frac{3}{4}-\frac{r}{R}\right) & \text { for } r \leq R \\ \text { Zero } & \text { for } r>R\end{array}\right.$
Where, $r ( r < R )$ is the distance from the centre $O$ (as shown in figure). The electric field at point $P$ will be.