14πϵ0Qr\dfrac{1}{4\pi \epsilon _0}\dfrac{Q}{r}4πϵ01rQ
4π∈0r4\pi \in _0r4π∈0r
14πϵ0Qr2\dfrac{1}{4\pi \epsilon _0}\dfrac{Q}{r^2}4πϵ01r2Q