Charge is distributed within a sphere of radius $R$ with a volume charge density $\rho (r) = \frac{A}{{{r^2}}}{e^{ - 2r/a}}$ where $A$ and $a$ are constants. If $Q$ is the total charge of this charge distribution, the radius $R$ is.
$a\,\log \,\left( {1 - \frac{Q}{{2\pi aA}}} \right)$
$\frac{a}{2}\,\log \,\left( {\frac{1}{{1 - \frac{Q}{{2\pi aA}}}}} \right)$
$a\,\log \,\left( {\frac{1}{{1 - \frac{Q}{{2\pi aA}}}}} \right)$
$\frac{a}{2}\,\log \left( {1 - \frac{1}{{2\pi aA}}} \right)\,$
If volume charge density is $\rho $, then what will be the charge on $\Delta V$ volume ?
A solid sphere of radius $R_1$ and volume charge density $\rho = \frac{{{\rho _0}}}{r}$ is enclosed by a hollow sphere of radius $R_2$ with negative surface charge density $\sigma $, such that the total charge in the system is zero. $\rho_0$ is a positive constant and $r$ is the distance from the centre of the sphere. The ratio $R_2/R_1$ is
Two isolated metallic spheres of radii $2 \,cm$ and $4 \,cm$ are given equal charge, then the ratio of charge density on the surfaces of the spheres will be
In the absence of other conductors, the surface charge density
A semicircular ring of radius $'a'$ has charge density $\lambda = {\lambda _0}\,\cos \,\theta $ where ${\lambda _0}$ is constant and $'\theta'$ is shown in figure. Then total charge on the ring is