	Standard:	Linked to collision space-time:
Coulomb constant	$k_{e} = \frac{1}{4 π}$	$k_{e} = \frac{1}{4 π}$
Planck charge	$q_{p} = \sqrt{4 π ℏ c}$	${\bar{q}}_{p} = l_{p} \sqrt{4 π c}$
Planck voltage	$V_{p} = \frac{\sqrt{ℏ c}}{l_{p} \sqrt{4 π}}$	${\bar{V}}_{p} = \frac{1}{\sqrt{4 π c}}$
Planck energy	$E_{p} = V_{p} q_{p} = ℏ \frac{c}{l_{p}}$	${\bar{E}}_{p} = {\bar{V}}_{p} {\bar{q}}_{p} = l_{p}$
Planck impedance	$I_{p} = \frac{\sqrt{4 π ℏ c}}{l_{p}}$	${\bar{I}}_{p} = \frac{\sqrt{4 π}}{\sqrt{c}}$
Planck resistance	$R_{Ω} = \frac{V_{p}}{I_{p}} = c$	${\bar{R}}_{Ω} = \frac{V_{p}}{I_{p}} = c$
Magnetic field	$\sqrt{\frac{1}{4 π} \frac{c^{5}}{ℏ G^{2}}} = \frac{\sqrt{ℏ c \times 10^{- 7}}}{\sqrt{4 π} l_{p}^{2}}$	$\frac{\sqrt{c}}{\sqrt{4 π} l_{p}}$
Electric field	$\sqrt{\frac{1}{4 π} \frac{c^{7}}{ℏ G^{2}}} = \frac{c \sqrt{ℏ c}}{\sqrt{4 π} l_{p}^{2}}$	$\frac{c \sqrt{c}}{\sqrt{4 π} l_{p}}$
Coulomb force Planck charges	$F = \frac{1}{4 π} \frac{q_{p} q_{p}}{r^{2}} = ℏ \frac{c}{r^{2}}$	$\bar{F} = \frac{1}{4 π} \frac{{\bar{q}}_{p} {\bar{q}}_{p}}{r^{2}} = c \frac{4 π l_{p}^{2}}{4 π r^{2}} = \frac{l_{p}^{2}}{r^{2}} c$
Charged square	$q_{p}^{2} = 4 π c ℏ$	${\bar{q}}_{p}^{2} = c 4 π l_{p}^{2}$