Editing Gaussian units (section)

=== Other basic laws ===

{| class="wikitable plainrowheaders"
|+ Other electromagnetic laws in Gaussian system and ISQ
|-
! scope="col" | Name
! scope="col" | Gaussian system
! scope="col" | {{abbr|ISQ|International System of Quantities}}
|-
! scope="row" | [[Lorentz force]]
| <math>\mathbf{F} = q^{_\mathrm{G}}\,\left(\mathbf{E}^{_\mathrm{G}}+\tfrac{1}{c}\,\mathbf{v}\times\mathbf{B}^{_\mathrm{G}}\right)</math>
| <math>\mathbf{F} = q^{_\mathrm{I}}\,\left(\mathbf{E}^{_\mathrm{I}}+\mathbf{v}\times\mathbf{B}^{_\mathrm{I}}\right)</math>
|-
! scope="row" | [[Coulomb's law]]
| <math>\mathbf{F} = \frac{q^{_\mathrm{G}}_1 q^{_\mathrm{G}}_2}{r^2}\,\mathbf{\hat r}</math>
| <math>\mathbf{F} = \frac{1}{4\pi\varepsilon_0}\,\frac{q^{_\mathrm{I}}_1 q^{_\mathrm{I}}_2}{r^2}\, \mathbf{\hat r}</math> <br />
|-
! scope="row" | Electric field of<br />[[Coulomb's law|stationary point charge]]
| <math>\mathbf{E}^{_\mathrm{G}} = \frac{q^{_\mathrm{G}}}{r^2}\,\mathbf{\hat r}</math>
| <math>\mathbf{E}^{_\mathrm{I}} = \frac{1}{4\pi\varepsilon_0}\,\frac{q^{_\mathrm{I}}}{r^2}\,\mathbf{\hat r}</math>
|-
! scope="row" | [[Biot–Savart law]]<ref>[https://books.google.com/books?id=RvZFuqw6mXEC&pg=PA180 Introduction to Electrodynamics by Capri and Panat, p180]</ref>
| <math> \mathbf{B}^{_\mathrm{G}} = \frac{1}{c}\!\oint\frac{I^{_\mathrm{G}} \times \mathbf{\hat r}}{r^2}\,\operatorname{d}\!\mathbf{\boldsymbol{\ell}}</math>
| <math> \mathbf{B}^{_\mathrm{I}} = \frac{\mu_0}{4\pi}\!\oint\frac{I^{_\mathrm{I}} \times \mathbf{\hat r}}{r^2}\,\operatorname{d}\!\mathbf{\boldsymbol{\ell}}</math>
|-
! scope="row" | [[Poynting vector]]<br />(microscopic)
| <math>\mathbf{S} = \frac{c}{4\pi}\,\mathbf{E}^{_\mathrm{G}} \times \mathbf{B}^{_\mathrm{G}}</math>
| <math>\mathbf{S} = \frac{1}{\mu_0}\,\mathbf{E}^{_\mathrm{I}} \times \mathbf{B}^{_\mathrm{I}}</math>
|}