n2 h2ϵ0πme\frac{\mathrm{n}^{2} \mathrm{~h}^{2} \epsilon_{0}}{\pi \mathrm{me}}πmen2 h2ϵ0
me48n2h2ϵ02\frac{m e^{4}}{8 n^{2} h^{2} \epsilon_{0}^{2}}8n2h2ϵ02me4
e4πϵomrn\frac{\mathrm{e}}{\sqrt{4 \pi \epsilon_{\mathrm{o}} \mathrm{mr}_{\mathrm{n}}}}4πϵomrne
e4π∈omrn\frac{\mathrm{e}}{4 \pi \in_{\mathrm{o}} \mathrm{mr}_{\mathrm{n}}}4π∈omrne