title: Heaviside–Lorentz units
text: Heaviside–Lorentz units (or Lorentz–Heaviside units) constitute a system of units and quantities that extends the CGS with a particular set of equations that defines electromagnetic quantities, named for Oliver Heaviside and Hendrik Antoon Lorentz. They share with the CGS-Gaussian system that the electric constant  and magnetic constant  do not appear in the defining equations for electromagnetism, having been incorporated implicitly into the electromagnetic quantities. Heaviside–Lorentz units may be thought of as normalizing  and , while at the same time revising Maxwell's equations to use the speed of light  instead.
  
  The Heaviside–Lorentz unit system, like the International System of Quantities upon which the SI system is based, but unlike the CGS-Gaussian system, is rationalized, with the result that there are no factors of  appearing explicitly in Maxwell's equations. That this system is rationalized partly explains its appeal in quantum field theory: the Lagrangian underlying the theory does not have any factors of  when this system is used. Consequently, electromagnetic quantities in the Heaviside–Lorentz system differ by factors of  in the definitions of the electric and magnetic fields and of electric charge.  It is often used in relativistic calculations, and are used in particle physics.  They are particularly convenient when performing calculations in spatial dimensions greater than three such as in string theory.
  
  Motivation 
  
  In the mid-late 19th Century, electromagnetic measurements were frequently made in either the so-called electrostatic (ESU) or electromagnetic (EMU) systems of units. These were based respectively on Coulomb's and Ampere's Law. Use of these systems, as with to the subsequently developed Gaussian CGS units, resulted in many factors of  appearing in formulas for electromagnetic results, including those without circular or spherical symmetry. For example, in the CGS-Gaussian system, the capacitance of sphere of radius  is  while that of a parallel plate capacitor is , where  is the area of the plates and  is their separation.
  
  Heaviside, who was an important, though somewhat isolated, early theorist of electromagnetism, suggested in 1882 that the irrational appearance of  in these sorts of relations could be removed by redefining the unit of the charges and fields.
  
  In 1893 Heaviside wrote
  
  Length–mass–time framework 
  
  As in the Gaussian system (), the Heaviside–Lorentz system () uses the length–mass–time dimensions. This means that all of the units of electric and magnetic quantities are expressible in terms of the units of the base quantities length, time and mass.
  
  Coulomb's equation, used to define charge in these systems, is  in the Gaussian system, and  in the HL system. The unit of charge then connects to , where 'HLC' is the HL unit of charge. The HL quantity  describing a charge is then  times larger than the corresponding Gaussian quantity. There are comparable relationships for the other electromagnetic quantities (see below).
  
  The commonly used set of units is the called the SI, which defines two constants, the vacuum permittivity () and the vacuum permeability (). These can be used to convert SI units to their corresponding Heaviside–Lorentz values, as detailed below.  For example, SI charge is .  When one puts , , , and , this evaluates to , the SI-equivalent of the Heaviside–Lorentz unit of charge.
  
  Comparison of Heaviside–Lorentz with other systems of units 
  
  This section has a list of the basic formulas of electromagnetism, given in the SI, Heaviside–Lorentz, and Gaussian systems.
  Here  and  are the electric field and displacement field, respectively,
   and  are the magnetic fields,
   is the polarization density,
   is the magnetization,
   is charge density,
   is current density,
   is the speed of light in vacuum,
   is the electric potential,
   is the magnetic vector potential,
   is the Lorentz force acting on a body of charge  and velocity ,
   is the permittivity,
   is the electric susceptibility,
   is the magnetic permeability, and
   is the magnetic susceptibility.
  
  Maxwell's equations 
  
  The electric and magnetic fields can be written in terms of the potentials  and .
  The definition of the magnetic field in terms of , , is the same in all systems of units, but the electric field is  in the SI system, but  in the HL or Gaussian systems.
  
  Other basic laws
  
  Dielectric and magnetic materials 
  
  Below are the expressions for the macroscopic fields , ,  and  in a material medium. It is assumed here for simplicity that the medium is homogeneous, linear, isotropic, and nondispersive, so that the susceptibilities are constants.
  
  Note that The quantities ,  and  are dimensionless, and they have the same numeric value. By contrast, the electric susceptibility  is dimensionless in all the systems, but has  for the same material:
  
  The same statements apply for the corresponding magnetic quantities.
  
  Advantages and disadvantages of Heaviside–Lorentz units
  
  Advantages 
  
   The formulas above are clearly simpler in  units compared to either  or Gaussian units. As Heaviside proposed, removing the  from the Gauss law and putting it in the Force law considerably reduces the number of places the  appears compared to Gaussian CGS units.
   Removing the explicit  from the Gauss law makes it clear that the inverse-square force law arises by the  field spreading out over the surface of a sphere. This allows a straightforward extension to other dimensions. For example the case of long, parallel wires extending straight in the  direction can be considered a two-dimensional system. Another example is in string theory, where more than three spatial dimensions often need to be considered.
   The equations are free of the constants  and  that are present in the SI system. (In addition  and  are overdetermined, because .)
  
  The below points are true in both Heaviside–Lorentz and Gaussian systems, but not SI.
  
   The electric and magnetic fields  and  have the same dimensions in the Heaviside–Lorentz system, meaning it is easy to recall where factors of  go in the Maxwell equation. Every time derivative comes with a , which makes it dimensionally the same as a space derivative. In contrast, in SI units  is .
   Giving the  and  fields the same dimension makes the assembly into the electromagnetic tensor more transparent. There are no factors of  that need to be inserted when assembling the tensor out of the three-dimensional fields. Similarly,  and  have the same dimensions and are the four components of the 4-potential.
   The fields , , , and  also have the same dimensions as  and . For vacuum, any expression involving  can simply be recast as the same expression with . In SI units,  and  have the same units, as do  and , but they have different units from each other and from  and .
  
  Disadvantages 
  
   Despite Heaviside's urgings, it proved difficult to persuade people to switch from the established units. He believed that if the units were changed, "[o]ld style instruments would very soon be in a minority, and then disappear ...". Persuading people to switch was already difficult in 1893, and in the meanwhile there have been more than a century's worth of additional textbooks printed and voltmeters built.
  
   Heaviside–Lorentz units, like the Gaussian CGS units by which they generally differ by a factor of about 3.5, are frequently of rather inconvenient sizes. The ampere (coulomb/second) is reasonable unit for measuring currents commonly encountered, but the ESU/s, as demonstrated above, is far too small. The Gaussian CGS unit of electric potential is named a statvolt. It is about , a value which is larger than most commonly encountered potentials. The henry, the SI unit for inductance is already on the large side compared to most inductors; the Gaussian unit is 12 orders of magnitude larger.
  
   A few of the Gaussian CGS units have names; none of the Heaviside–Lorentz units do.
  
  Textbooks in theoretical physics use Heaviside–Lorentz units nearly exclusively, frequently in their natural form (see below),  system's conceptual simplicity and compactness significantly clarify the discussions, and it is possible if necessary to convert the resulting answers to appropriate units after the fact by inserting appropriate factors of  and . Some textbooks on classical electricity and magnetism have been written using Gaussian CGS units, but recently some of them have been rewritten to use SI units. Outside of these contexts, including for example magazine articles on electric circuits, Heaviside–Lorentz and Gaussian CGS units are rarely encountered.
  
  Translating expressions and formulas between systems
  
  To convert any expression or formula between the SI, Heaviside–Lorentz or Gaussian systems, the corresponding quantities shown in the table below can be directly equated and hence substituted. This will reproduce any of the specific formulas given in the list above.
  
  As an example, starting with the equation
  
  and the equations from the table
  
  Moving the factor across in the latter identities and substituting, the result is
  
  which then simplifies to
  
  Notes
  
  References 
  
  Special relativity
  Electromagnetism
  Hendrik Lorentz