Table of Electromagnetic Quantities and Their Units

The table below lists quantities that appear in the equations of natural law related to electromagnetic phenomena. For each, the table includes the typical formulaic symbol for the quantity, the conventional terminology used to refer to it, in some cases alternative terminology which Primel introduces, along with the coherent unit provided by SI, the coherent unit (quantitel) provided by Primel, and the conversion from the Primel unit to SI units.

Quantity Symbol	Conventional Terminology Primel Terminology	SI Unit Primel Unit Primel conversion to SI
	electric charge quantity of electricity	coulomb = C ⚀electrel ≈ 58.3547142537770_d μC
	magnetic pole strength magnetic charge quantity of magnetism	C·m·s⁻¹ = A·m ⚀magnetel = ⚀electrel × ⚀velocitel ≈ (1.65414607212326×10⁻⁵)_d A·m
	electric current	ampere = A ⚀currentel = ⚀electrel / ⚀timel = ⚀magnetel / ⚀lengthel ≈ 2.01673892461053_d mA
	magnetic scalar potential magnetism gradient
	alternation	A·s⁻¹ = C·s⁻² ⚀alternationel = ⚀currentel / ⚀timel = ⚀electrel / ⚀timel² ≈ (6.96984972345401×10⁻²)_dA·s⁻¹
	electric displacement field free electrization	C·m⁻² ⚀electrizationel = ⚀areanelic·electrel = ⚀electrel / ⚀areanel ≈ (8.67416326062990×10⁻¹)_d C·m⁻²
	polarization density material electrization
	magnetizing field free magnetization	(A·m)·m⁻²= A·m⁻¹ ⚀magnetizationel = ⚀areanelic·magnetel = ⚀magnetel / ⚀areanel ≈ (2.45881301451119×10⁻¹)_d A·m⁻¹
	bound magnetization material magnetization
	charge density electrodensity	C·m⁻³ ⚀electrodensitel = ⚀volumelic·electrel = ⚀electrel / ⚀volumel ≈ (1.05755609984820×10²)_d C·m⁻³
	electric displacement gradient free electrodensity
	polarization density gradient material electrodensity
	current density magnetodensity	(A·m)·m⁻³= A·m⁻² ⚀magnetodensitel = ⚀volumelic·magnetel = ⚀magnetel / ⚀volumel ≈ 2.99779082287369×10¹ A·m⁻²
	magnetizing field gradient free magnetodensity
	bound magnetization gradient material magnetodensity
	electric field electric force	N·C⁻¹= V·m⁻¹ ⚀electrelic·forcel = ⚀forcel / ⚀electrel ≈ (9.26309397578308×10¹)_dN·C⁻¹
	magnetic flux density magnetic force	tesla = T = N·(A·m)⁻¹= Wb·m⁻² = kg·s⁻²·A⁻¹ ⚀magnetelic·forcel = ⚀forcel / ⚀magnetel ≈ (3.26782024376396×10²)_dT
	electric flux electric influence	N·m²·C⁻¹ = V·m ⚀electrelic·influencel = ⚀influencel / ⚀electrel = ⚀forcel × ⚀areanel / ⚀electrel ≈ (6.23166968180227×10⁻³)_d V·m
	magnetic flux magnetic influence	weber = Wb = N·m²·(A·m)⁻¹ = J·A⁻¹= V·s ⚀magnetelic·influencel = ⚀influencel / ⚀magnetel = ⚀forcel × ⚀areanel / ⚀magnetel ≈ (2.19839897898932×10⁻²)_d Wb
	electric potential electric potential	volt = V = J·C⁻¹ = W·A⁻¹= A·Ω ⚀electrelic·potentialel = ⚀εpotel = ⚀potentialel / ⚀electrel ≈ (7.59766687138707×10⁻¹)_d V
	magnetic vector potential magnetic potential	J·(A·m)⁻¹ = N·A⁻¹ = V·s = Wb·m⁻¹ = T·m ⚀magnetelic·potentialel = ⚀μpotel = ⚀potentialel / ⚀magnetel ≈ 2.68029339577057_d Wb·m⁻¹
	magnetic vector potential magnetic potential
	electric field divergence electric tension	N·m⁻¹·C⁻¹= V·m⁻² ⚀electrelic·tensionel = ⚀tensionel / ⚀electrel = ⚀forcel / ⚀lengthel / ⚀electrel ≈ (1.12935867624483×10⁴)_d N·m⁻¹·C⁻¹
	electric field curl electric tension
	electric field Laplacian electric pressure	N·m⁻²·C⁻¹= Pa·C⁻¹= V·m⁻³ ⚀electrelic·pressurel = ⚀pressurel / ⚀electrel = ⚀forcel / ⚀areanel / ⚀electrel ≈ 1.37691685191140×10⁶ Pa·C⁻¹
	magnetic field divergence magnetic tension	T·m⁻¹ = N·m⁻¹·(A·m)⁻¹= Wb·m⁻³ = kg·m⁻¹·s⁻²·A⁻¹ ⚀magnetelic·tensionel = ⚀tensionel / ⚀magnetel = ⚀forcel / ⚀lengthel / ⚀magnetel ≈ (3.98413440946584×10⁴)_dT·m⁻¹
	magnetic field curl magnetic tension
	magnetic field Laplacian magnetic pressure	T·m⁻² = N·m⁻²·(A·m)⁻¹= kg·m⁻²·s⁻²·A⁻¹ ⚀magnetelic·pressurel = ⚀pressurel / ⚀magnetel = ⚀forcel / ⚀areanel / ⚀magnetel ≈ (4.85746638695353×10⁶)_dT·m⁻²
	elastance	F⁻¹ = J·C⁻² ⚀elastancel ≈ 1.30197996315187×10⁴ F⁻¹
	capacitance	F = C²·J⁻¹ ⚀capacitancel ≈ 7.68060975054616×10⁻⁵ F
	inductance	henry = H = J·A⁻² = Wb·A⁻¹ ⚀inductancel ≈ (1.09007613834491×10¹)_d H
	reluctance	H⁻¹ = J⁻¹·A² = Wb⁻¹·A ⚀reluctancel ≈ (9.17367113014993×10⁻²)_d H⁻¹
	reciprocal permittivity elastivity	m·F⁻¹ = N·m²·C⁻² ⚀elastivitel = ⚀squarelectrelic·influencel ≈ (1.06789481561019×10²)_d m·F⁻¹
	permittivity capacitivity	F·m⁻¹= N⁻¹·m⁻²·C² ⚀capacitivitel = ⚀influencelic·squarelectrel ≈ (9.36421813630215×10⁻³)_d F·m⁻¹
	permeability inductivity	H·m⁻¹= N·m²·(A·m)⁻² = N·A⁻² ⚀inductivitel = ⚀squaremagnetelic·influencel ≈ (1.32902348591708×10³)_d H·m⁻¹
	reciprocal permeability reluctivity	m·H⁻¹= N⁻¹·m⁻²·(A·m)² = N⁻¹·A² ⚀reluctivitel = ⚀influencelic·squaremagnetel ≈ (7.52432150820839×10⁻⁴)_d m·H⁻¹
	resistance	ohm = Ω ⚀resistancel ≈ (3.76730313412×10²)_d Ω
	reactance	ohm = Ω ⚀reactancel ≈ (3.76730313412×10²)_d Ω
	impedance	ohm = Ω impedancel ≈ (3.76730313412×10²)_d Ω
	conductance	siemens = S ⚀conductancel ≈ (2.65441872978875×10⁻³)_d S
	susceptance	siemens = S ⚀susceptancel ≈ (2.65441872978875×10⁻³)_d S
	admittance	siemens = S ⚀admittancel ≈ (2.65441872978875×10⁻³)_d S
	resistivity	Ω·m ⚀resistivitel = ⚀resistancel × ⚀lengthel ≈ 3.08997342479801_d Ω·m
	conductivity	S·m⁻¹ ⚀conductivitel = ⚀rconductancel / ⚀lengthel ≈ (3.23627378790603×10⁻¹)_d S·m⁻¹