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## Summary

In physics, natural units are physical units of measurement based only on universal physical constants. For example, the elementary charge e is a natural unit of electric charge, and the speed of light c is a natural unit of speed. A purely natural system of units has all of its units usually defined such that the numerical values of the selected physical constants in terms of these units are exactly 1. These constants may then be omitted from mathematical expressions of physical laws, and while this has the apparent advantage of simplicity, it may entail a loss of clarity due to the loss of information for dimensional analysis. It precludes the interpretation of an expression in terms of fundamental physical constants, such as e and c, unless it is known which units (in dimensionful units) the expression is supposed to have. In this case, the reinsertion of the correct powers of e, c, etc., can be uniquely determined.

## Systems of natural units

### Planck units

Quantity Expression Metric value Name
Length (L) $l_{\text{P}}={\sqrt {\hbar G \over c^{3}}}$  1.616×10−35 m Planck length
Mass (M) $m_{\text{P}}={\sqrt {\hbar c \over G}}$  2.176×10−8 kg Planck mass
Time (T) $t_{\text{P}}={\sqrt {\hbar G \over c^{5}}}$  5.391×10−44 s Planck time
Temperature (Θ) $T_{\text{P}}={\sqrt {\frac {\hbar c^{5}}{G{k_{\text{B}}}^{2}}}}$  1.417×1032 K Planck temperature

The Planck unit system uses the following constants to have numeric value 1 in terms of the resulting units:

c, ℏ, G, kB,

where c is the speed of light, is the reduced Planck constant, G is the gravitational constant, and kB is the Boltzmann constant.

Planck units are a system of natural units that is not defined in terms of properties of any prototype, physical object, or even elementary particle. They only refer to the basic structure of the laws of physics: c and G are part of the structure of spacetime in general relativity, and captures the relationship between energy and frequency which is at the foundation of quantum mechanics. This makes Planck units particularly useful and common in theories of quantum gravity, including string theory.[citation needed]

Planck considered only the units based on the universal constants G, h, c, and kB to arrive at natural units for length, time, mass, and temperature, but no electromagnetic units. The Planck system of units is now understood to use the reduced Planck constant, , in place of the Planck constant, h.

### Stoney units

Quantity Expression Metric value
Length (L) $l_{\text{S}}={\sqrt {\frac {Gk_{\text{e}}e^{2}}{c^{4}}}}$  1.38068×10−36 m
Mass (M) $m_{\text{S}}={\sqrt {\frac {k_{\text{e}}e^{2}}{G}}}$  1.85921×10−9 kg
Time (T) $t_{\text{S}}={\sqrt {\frac {Gk_{\text{e}}e^{2}}{c^{6}}}}$  4.60544×10−45 s
Electric charge (Q) $q_{\text{S}}=e\$  1.60218×10−19 C

The Stoney unit system uses the following constants to have numeric value 1 in terms of the resulting units:

c, G, ke, e,

where c is the speed of light, G is the gravitational constant, ke is the Coulomb constant, and e is the elementary charge.

George Johnstone Stoney's unit system preceded that of Planck. He presented the idea in a lecture entitled "On the Physical Units of Nature" delivered to the British Association in 1874. Stoney units did not consider the Planck constant, which was discovered only after Stoney's proposal.

Stoney units are rarely used in modern physics for calculations, but they are of historical interest.

### Atomic units

Quantity Expression Metric value
Length (L) $l_{\text{A}}={\frac {(4\pi \epsilon _{0})\hbar ^{2}}{m_{\text{e}}e^{2}}}$  5.292×10−11 m
Mass (M) $m_{\text{A}}=m_{\text{e}}$  9.109×10−31 kg
Time (T) $t_{\text{A}}={\frac {(4\pi \epsilon _{0})^{2}\hbar ^{3}}{m_{\text{e}}e^{4}}}$  2.419×10−17 s
Electric charge (Q) $q_{\text{A}}=e$  1.602×10−19 C

The Hartree atomic unit system uses the following constants to have numeric value 1 in terms of the resulting units:

e, me, ℏ, ke.

Coulomb's constant, ke, is generally expressed as 1/4πε0 when working with this system.

These units are designed to simplify atomic and molecular physics and chemistry, especially the hydrogen atom, and are widely used in these fields. The Hartree units were first proposed by Douglas Hartree.

The units are designed especially to characterize the behavior of an electron in the ground state of a hydrogen atom. For example, in Hartree atomic units, in the Bohr model of the hydrogen atom an electron in the ground state has orbital radius (the Bohr radius) a0 = 1 lA, orbital velocity = 1 lAtA−1, angular momentum = 1 mAlAtA−1, ionization energy = 1/2 mAlA2tA−2, etc.

The unit of energy is called the Hartree energy in the Hartree system. The speed of light is relatively large in Hartree atomic units (c = 1/α lAtA−1 ≈ 137 lAtA−1) since an electron in hydrogen tends to move much slower than the speed of light. The gravitational constant is extremely small in atomic units (G ≈ 10−45 mA−1lA3tA−2), which is due to the gravitational force between two electrons being far weaker than the Coulomb force between them.

A less commonly used closely related system is the system of Rydberg atomic units, in which e2/2, 2me, ℏ, ke are used as the normalized constants, with resulting units lR = a0 = (4πε0)2/mee2, tR = 2(4πε0)23/mee4, mR = 2me, qR = e2.

### Natural units (particle and atomic physics)

Quantity Expression Metric value
Length (L) ${\frac {\hbar }{m_{\text{e}}c}}$  3.862×10−13 m
Mass (M) $m_{\text{e}}\$  9.109×10−31 kg
Time (T) ${\frac {\hbar }{m_{\text{e}}c^{2}}}$  1.288×10−21 s
Electric charge (Q) ${\sqrt {\varepsilon _{0}\hbar c}}$  5.291×10−19 C

The natural unit system, used only in the fields of particle and atomic physics, uses the following constants to have numeric value 1 in terms of the resulting units:: 126

c, me, ℏ, ε0,

where c is the speed of light, me is the electron mass, is the reduced Planck constant, and ε0 is the vacuum permittivity.

The vacuum permittivity ε0 is implicitly normalized, as is evident from the physicists' expression for the fine-structure constant, written α = e2/(4π), which may be compared to the same expression in SI: α = e2/(4πε0c).: 128

### Quantum chromodynamics units

Quantity Expression Metric value
Length (L) $l_{\mathrm {QCD} }={\frac {\hbar }{m_{\text{p}}c}}$  2.103×10−16 m
Mass (M) $m_{\mathrm {QCD} }=m_{\text{p}}\$  1.673×10−27 kg
Time (T) $t_{\mathrm {QCD} }={\frac {\hbar }{m_{\text{p}}c^{2}}}$  7.015×10−25 s
Electric charge (Q) $q_{\mathrm {QCD} }=e$  (original) 1.602×10−19 C
$q_{\mathrm {QCD} }={\frac {e}{\sqrt {4\pi \alpha }}}$  (rat.) 5.291×10−19 C
$q_{\mathrm {QCD} }={\frac {e}{\sqrt {\alpha }}}$  (non-rat.) 1.876×10−18 C
c = mp = ℏ = 1; if rationalized, then $\epsilon _{0}$  is 1, if not, $4\pi \epsilon _{0}$  is 1 (in the original QCD units, e is 1 instead.[citation needed])

The electron rest mass is replaced with that of the proton. Strong units, also called quantum chromodynamics (QCD) units, are "convenient for work in QCD and nuclear physics, where quantum mechanics and relativity are omnipresent and the proton is an object of central interest".

### Geometrized units

c = G = 1

The geometrized unit system, used in general relativity, is an incompletely defined system. In this system, the base physical units are chosen so that the speed of light and the gravitational constant are set equal to unity. Other units may be treated however desired. Planck units and Stoney units are examples of geometrized unit systems.

### Summary table

Quantity / Symbol Planck Stoney Hartree Rydberg particle and atomic physics rationalized QCD non-rationalized QCD
Defining constants $c$ , $G$ , $\hbar$ , $k_{\text{B}}$  $c$ , $G$ , $e$ , $k_{\text{e}}$  $e$ , $m_{\text{e}}$ , $\hbar$ , $k_{\text{e}}$  $e^{2}/2$ , $2m_{\text{e}}$ , $\hbar$ , $k_{\text{e}}$  $c$ , $m_{\text{e}}$ , $\hbar$ , $\varepsilon _{0}$  $c$ , $m_{\text{p}}$ , $\hbar$ , $\varepsilon _{0}$  $c$ , $m_{\text{p}}$ , $\hbar$ , $4\pi \varepsilon _{0}$
Speed of light
$c$
$1$  $1$  ${\frac {1}{\alpha }}$  ${\frac {2}{\alpha }}$  $1$  $1$  $1$
Reduced Planck constant
$\hbar ={\frac {h}{2\pi }}$
$1$  ${\frac {1}{\alpha }}$  $1$  $1$  $1$  $1$  $1$
Elementary charge
$e$
$-$  $1$  $1$  ${\sqrt {2}}$  ${\sqrt {4\pi \alpha }}$  ${\sqrt {4\pi \alpha }}$  ${\sqrt {\alpha }}$
Vacuum permittivity
$\varepsilon _{0}$
$-$  ${\frac {1}{4\pi }}$  ${\frac {1}{4\pi }}$  ${\frac {1}{4\pi }}$  $1$  $1$  ${\frac {1}{4\pi }}$
Coulomb constant
$k_{\text{e}}$
$-$  $1$  $1$  $1$  ${\frac {1}{4\pi }}$  ${\frac {1}{4\pi }}$  $1$
Gravitational constant
$G$
$1$  $1$  ${\frac {\alpha _{\mathrm {G} }}{\alpha }}$  ${\frac {8\alpha _{\mathrm {G} }}{\alpha }}$  $\alpha _{\mathrm {G} }$  $\mu ^{2}\alpha _{\mathrm {G} }$  $\mu ^{2}\alpha _{\mathrm {G} }$
Boltzmann constant
$k_{\text{B}}$
$1$  $-$  $-$  $-$  $-$  $-$  $-$
Electron mass
$m_{\text{e}}$
${\sqrt {\alpha _{\mathrm {G} }}}$  ${\sqrt {\frac {\alpha _{\mathrm {G} }}{\alpha }}}$  $1$  ${\frac {1}{2}}$  $1$  ${\frac {1}{\mu }}$  ${\frac {1}{\mu }}$
Proton mass
$m_{\text{p}}$
$\mu {\sqrt {\alpha _{\mathrm {G} }}}$  $\mu {\sqrt {\frac {\alpha _{\mathrm {G} }}{\alpha }}}$  $\mu$  ${\frac {\mu }{2}}$  $\mu$  $1$  $1$

where:

• α is the fine-structure constant (α = e2/4πε0ħc ≈ 0.007297)
• αG is the electron-electron Gravitational coupling constant (αG = G$m_{\text{e}}$ 2/ħc1.7518×10−45)
• μ is the Proton-to-electron mass ratio (μ1836.15267)
• A dash (–) indicates where the system is not sufficient to express the quantity.

## Notes and references

1. ^ "2018 CODATA Value: Planck length". The NIST Reference on Constants, Units, and Uncertainty. NIST. 20 May 2019. Retrieved 2019-05-20.
2. ^ "2018 CODATA Value: Planck mass". The NIST Reference on Constants, Units, and Uncertainty. NIST. 20 May 2019. Retrieved 2019-05-20.
3. ^ "2018 CODATA Value: Planck time". The NIST Reference on Constants, Units, and Uncertainty. NIST. 20 May 2019. Retrieved 2019-05-20.
4. ^ "2018 CODATA Value: Planck temperature". The NIST Reference on Constants, Units, and Uncertainty. NIST. 20 May 2019. Retrieved 2019-05-20.
5. ^ However, if it is assumed that at the time the Gaussian definition of electric charge was used and hence not regarded as an independent quantity, the Coulomb constant ke = 1/4πε0 would be implicitly added to the list of defining constants, this would yield a charge unit ħc/ke.
6. ^ Tomilin, K. A., 1999, "Natural Systems of Units: To the Centenary Anniversary of the Planck System", 287–296.
7. ^ Ray, T.P. (1981). "Stoney's Fundamental Units". Irish Astronomical Journal. 15: 152. Bibcode:1981IrAJ...15..152R.
8. ^ "Atomic Rydberg Units" (PDF).
9. ^ "2018 CODATA Value: natural unit of length". The NIST Reference on Constants, Units, and Uncertainty. NIST. 20 May 2019. Retrieved 2020-05-31.
10. ^ "2018 CODATA Value: natural unit of mass". The NIST Reference on Constants, Units, and Uncertainty. NIST. 20 May 2019. Retrieved 2020-05-31.
11. ^ "2018 CODATA Value: natural unit of time". The NIST Reference on Constants, Units, and Uncertainty. NIST. 20 May 2019. Retrieved 2020-05-31.
12. ^ International Bureau of Weights and Measures (2006), The International System of Units (SI) (PDF) (8th ed.), ISBN 92-822-2213-6, archived (PDF) from the original on 2021-06-04, retrieved 2021-12-16
13. ^ Frank Wilczek (2005), "On Absolute Units, I: Choices" (PDF), Physics Today, 58 (10): 12, Bibcode:2005PhT....58j..12W, doi:10.1063/1.2138392, retrieved 2020-05-31
14. ^ Frank Wilczek (2006), "On Absolute Units, II: Challenges and Responses" (PDF), Physics Today, 59 (1): 10, Bibcode:2006PhT....59a..10W, doi:10.1063/1.2180151, retrieved 2020-05-31
15. ^ International Bureau of Weights and Measures (2019-05-20), SI Brochure: The International System of Units (SI) (PDF) (9th ed.), ISBN 978-92-822-2272-0{{citation}}: CS1 maint: url-status (link)
16. ^ Wilczek, Frank (2007). "Fundamental Constants". arXiv:0708.4361 [hep-ph].