(d) $F = \frac{q_{1}q_{2}}{4\pi\varepsilon_{0}r^{2}}\ $
In a medium of dielectric constant, $\ K = \frac{\varepsilon}{\varepsilon_{0}}$s
$F' = \frac{q_{1}q_{2}}{4\pi\varepsilon_{0}r^{2}}$
As $F' = F$
$\therefore\ \ \ \ \frac{q_{1}q_{2}}{4\pi\varepsilon R^{2}} = \frac{q_{1}q_{2}}{4\pi\varepsilon_{0}r^{2}}\ $
$R^{2} = \frac{\ \varepsilon_{0}}{\varepsilon_{\ }}r^{2} = \frac{r^{2}}{K}$
$\therefore\ \ \ R = \frac{r}{\sqrt{K}}$