A spherically symmetric charge distribution is considered with charge density varying as is the distance from the centre O (as shown in figure). The electric field at point P will be:
\( \dfrac{\rho_0 r}{4\varepsilon_0}\left( \dfrac{3}{4} - \dfrac{r}{R} \right) \)
\( \dfrac{\rho_0 r}{3\varepsilon_0}\left( \dfrac{3}{4} - \dfrac{r}{R} \right) \)
\( \dfrac{\rho_0 r}{4\varepsilon_0}\left( 1 - \dfrac{r}{R} \right) \)
\( \dfrac{\rho_0 r}{5\varepsilon_0}\left( 1 - \dfrac{r}{R} \right) \)