F⃗=14πϵ0q1q2r2r⃗\vec{F}=\dfrac{1}{4\pi \epsilon _0}\dfrac{q_1q_2}{r^2}\vec{r}F=4πϵ01r2q1q2r
F⃗=14πϵ0q1q2r3r^\vec{F}=\dfrac{1}{4\pi \epsilon _0}\dfrac{q_1q_2}{r^3}\hat{r}F=4πϵ01r3q1q2r^
F⃗=14πϵ0q1q2r3r⃗\vec{F}=\dfrac{1}{4\pi \epsilon _0}\dfrac{q_1q_2}{r^3}\vec{r}F=4πϵ01r3q1q2r
F⃗=14πϵ0q1q2rr⃗\vec{F}=\dfrac{1}{4\pi \epsilon _0}\dfrac{q_1q_2}{r}\vec{r}F=4πϵ01rq1q2r