6 | | || $E = c E^{LH} = \frac{c }{\sqrt{4\pi}}E^{G}$ || |
7 | | || $\rho = \frac{1}{c}\rho^{LH} = \frac{\sqrt{4 \pi} }{c}\rho^{G}$|| |
8 | | || $J = \frac{1}{c} J^{LH} = \frac{\sqrt{4 \pi}}{c} J^{G}$|| |
9 | | || $B = B^{LH} = \frac{1}{\sqrt{4\pi}} B^{G}$ || |
| 6 | || AstroBEAR || Lorentz-Heaviside || Gaussian || Physical Units || |
| 7 | || $E $ || $ c E^{LH} $ || $ \frac{c }{\sqrt{4\pi}}E^{G}$ || $\mbox{g}^{1/2} \mbox{cm}^{1/2} \mbox{s}^{-2}$ || |
| 8 | || $\rho $ || $ \frac{1}{c}\rho^{LH} $ || $ \frac{\sqrt{4 \pi} }{c}\rho^{G}$ || $\mbox{g}^{1/2} \mbox{cm}^{-5/2}$ || |
| 9 | || $J$ || $\frac{1}{c} J^{LH} $ || $ \frac{\sqrt{4 \pi}}{c} J^{G}$ || $\mbox{g}^{1/2} \mbox{cm}^{-3/2} \mbox{s}^{-1}$ || |
| 10 | || $B$ || $B^{LH}$ || $\frac{1}{\sqrt{4\pi}} B^{G}$ || $\mbox{g}^{1/2} \mbox{cm}^{-1/2} \mbox{s}^{-1}$ || |