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
$\frac{{{\rho _o}r}}{{3{\varepsilon _0}}}\;\left( {\frac{5}{4} - \frac{r}{R}} \right)\;\;\;\;\;\;$
$\frac{{4\pi {\rho _0r}}}{{3{\varepsilon _0}}}\;\left( {\frac{5}{3} - \frac{r}{R}} \right)$
$\frac{{{\rho _o}r}}{{4{\varepsilon _0}}}\;\left( {\frac{5}{3} - \frac{r}{R}} \right)$
$\frac{{4\pi {\rho _0r}}}{{3{\varepsilon _0}}}\;\left( {\frac{5}{4} - \frac{r}{R}} \right)$
There is a solid sphere of radius $‘R’$ having uniformly distributed charge throughout it. What is the relation between electric field $‘E’$ and distance $‘r’$ from the centre ( $r$ is less than R ) ?
A long charged cylinder of linear charged density $\lambda$ is surrounded by a hollow co-axial conducting cylinder. What is the electric field in the space between the two cylinders?
According to Gauss’ Theorem, electric field of an infinitely long straight wire is proportional to
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 $\left( {K = \frac{1}{{4\pi {\varepsilon _0}}}} \right)$
Consider the force $F$ on a charge $'q'$ due to a uniformly charged spherical shell of radius $R$ carrying charge $Q$ distributed uniformly over it. Which one of the following statements is true for $F,$ if $'q'$ is placed at distance $r$ from the centre of the shell $?$