Electric field due to following configurations having charge density $\rho$

COLUMN - I		COLUMN - II
A)	At any interior point inside infinite plane sheet of charge	p)	0
B)	Infinite plane sheet of uniform thickness	q)	$\frac{\rho }{2{\epsilon }_0}$
C)	Non-conducting charged solid sphere of radius R at its surface	r)	$\frac{\mathrm{R}\rho }{3{\epsilon }_0}$
D)	Non-conducting charge solid sphere of radius R at its center	s)	$\frac{\rho }{{\epsilon }_0}$

A) At any interior point inside infinite plane sheet of charge E = 0

B) Net electric field at any point $\rho$ due to infinite plane sheet of uniform thickness

${\mathrm{E}}_{\mathrm{\rho }}={\mathrm{E}}_1-{\mathrm{E}}_2=\frac{\mathrm{\rho }\left(\frac{\mathrm{d}}{2}+\mathrm{x}\right)}{2{\mathrm{E}}_0}-\frac{\mathrm{\rho }\left(\frac{\mathrm{d}}{2}-\mathrm{x}\right)}{2{\mathrm{E}}_0}$

$\Rightarrow \mathrm{E}=\frac{\rho x}{{\mathrm{E}}_0}$

C) The intensity of electric field due to non conducting sphere $\mathrm{E}=\frac{1}{4\pi {ϵ}_0}\frac{\mathrm{Qr}}{{\mathrm{R}}^3}$

Interms of charge density $\mathrm{E}=\frac{1}{4{\mathrm{\pi ϵ}}_0}\left(\frac{\mathrm{\rho }\frac{4}{3}{\mathrm{\pi R}}^3}{{\mathrm{R}}^3}\right)\mathrm{r}\Rightarrow \mathrm{E}=\frac{\mathrm{\rho r}}{3{\mathrm{ϵ}}_0}$

on the surface r = R So $\mathrm{E}=\frac{\mathrm{\rho R}}{3{\mathrm{ϵ}}_0}$

D) When sphere is charged it lies only on external surface and the charge inside the sphere is zero so E = 0