# Planck units

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In particle physics and physical cosmology, Planck units are a set of units of measurement defined exclusively in terms of five universal physical constants, in such a manner that these five physical constants take on the numerical value of 1 when expressed in terms of these units.

Originally proposed in 1899 by German physicist Max Planck, these units are also known as natural units because the origin of their definition comes only from properties of nature and not from any human construct (e.g. luminous intensity, luminous flux, and equivalent dose). Planck units are only one system of several systems of natural units, but Planck units are not based on properties of any prototype object or particle (e.g. elementary charge, electron rest mass, and proton rest mass) (that would be arbitrarily chosen), but rather on only the properties of free space. Planck units have significance for theoretical physics since they simplify several recurring algebraic expressions of physical law by nondimensionalization. They are relevant in research on unified theories such as quantum gravity.

The term Planck scale refers to the magnitudes of space, time, energy and other units, below which (or beyond which) the predictions of the Standard Model, quantum field theory and general relativity are no longer reconcilable, and quantum effects of gravity are expected to dominate. This region may be characterized by energies around 1.96×109 J (the Planck energy), time intervals around 5.39×10−44 s (the Planck time) and lengths around 1.62×10−35 m (the Planck length). At the Planck scale, current models are not expected to be a useful guide to the cosmos, and physicists have no scientific model to suggest how the physical universe behaves. The best known example is represented by the conditions in the first 10−43 seconds of our universe after the Big Bang, approximately 13.8 billion years ago.

There are two versions of Planck units, Lorentz–Heaviside version and Gaussian version.

The five universal constants that Planck units, by definition, normalize to 1 are:

Each of these constants can be associated with a fundamental physical theory or concept: c with special relativity, G with general relativity, ħ with quantum mechanics, ε0 with electromagnetism, and kB with the notion of temperature/energy (statistical mechanics and thermodynamics).

## Introduction

Any system of measurement may be assigned a mutually independent set of base quantities and associated base units, from which all other quantities and units may be derived. In the International System of Units, for example, the SI base quantities include length with the associated unit of the metre. In the system of Planck units, a similar set of base quantities may be selected, and the Planck base unit of length is then known simply as the Planck length, the base unit of time is the Planck time, and so on. These units are derived from the five dimensional universal physical constants of Table 1, in such a manner that these constants are eliminated from fundamental selected equations of physical law when physical quantities are expressed in terms of Planck units. For example, Newton's law of universal gravitation,

{\displaystyle {\begin{aligned}F&=G{\frac {m_{1}m_{2}}{r^{2}}}\\\\&=\left({\frac {F_{\text{P}}l_{\text{P}}^{2}}{m_{\text{P}}^{2}}}\right){\frac {m_{1}m_{2}}{r^{2}}}\\\end{aligned}}}

can be expressed as:

${\displaystyle {\frac {F}{F_{\text{P}}}}={\frac {\left({\dfrac {m_{1}}{m_{\text{P}}}}\right)\left({\dfrac {m_{2}}{m_{\text{P}}}}\right)}{\left({\dfrac {r}{l_{\text{P}}}}\right)^{2}}}.}$

Both equations are dimensionally consistent and equally valid in any system of units, but the second equation, with G missing, is relating only dimensionless quantities since any ratio of two like-dimensioned quantities is a dimensionless quantity. If, by a shorthand convention, it is understood that all physical quantities are expressed in terms of Planck units, the ratios above may be expressed simply with the symbols of physical quantity, without being scaled explicitly by their corresponding unit:

${\displaystyle F={\frac {m_{1}m_{2}}{r^{2}}}\ .}$

This last equation (without G) is valid only if F, m1, m2, and r are the dimensionless numerical values of these quantities measured in terms of Planck units. This is why Planck units or any other use of natural units should be employed with care. Referring to G = c = 1, Paul S. Wesson wrote that, "Mathematically it is an acceptable trick which saves labour. Physically it represents a loss of information and can lead to confusion."[1]

## Definition

Table 1: Dimensional universal physical constants normalized with Planck units
Constant Symbol Dimension Value (SI units)[2]
Speed of light in vacuum c L T −1 2.99792458×108 m⋅s−1
(exact by definition of metre)
Gravitational constant G
(1 for the Gaussian version, 1/4π for the Lorentz–Heaviside version)
L3 M−1 T −2 6.67430(15)×10−11 m3⋅kg−1⋅s−2[3]
Reduced Planck constant ħ = h/2π
where h is the Planck constant
L2 M T −1 1.054571817...×10−34 J⋅s[4]
(exact by definition of the kilogram since 20 May 2019)
Coulomb constant ke = 1/4πε0
where ε0 is the vacuum permittivity
(1 for the Gaussian version, 1/4π for the Lorentz–Heaviside version)
L3 M T −2 Q−2 8.9875517873681764×109 kg⋅m3⋅s−4⋅A−2
(exact by definitions of ampere and metre until 20 May 2019)
Boltzmann constant kB L2 M T −2 Θ−1 1.380649×10−23 J⋅K−1[5]
(exact by definition of the kelvin since 20 May 2019)

Key: L = length, M = mass, T = time, I = electric current, Θ = temperature.

As can be seen above, the gravitational attractive force of two bodies of 1 Planck mass each, set apart by 1 Planck length is 1 Planck force. Likewise, the distance traveled by light during 1 Planck time is 1 Planck length. To determine, in terms of SI or another existing system of units, the quantitative values of the five base Planck units, those two equations and three others must be satisfied:

${\displaystyle l_{\text{P}}=c\ t_{\text{P}}}$
${\displaystyle F_{\text{P}}={\frac {m_{\text{P}}l_{\text{P}}}{t_{\text{P}}^{2}}}=4\pi G\ {\frac {m_{\text{P}}^{2}}{l_{\text{P}}^{2}}}}$ (Lorentz–Heaviside version)
${\displaystyle F_{\text{P}}={\frac {m_{\text{P}}l_{\text{P}}}{t_{\text{P}}^{2}}}=G\ {\frac {m_{\text{P}}^{2}}{l_{\text{P}}^{2}}}}$ (Gaussian version)
${\displaystyle E_{\text{P}}={\frac {m_{\text{P}}l_{\text{P}}^{2}}{t_{\text{P}}^{2}}}=\hbar \ {\frac {1}{t_{\text{P}}}}}$
${\displaystyle F_{\text{P}}={\frac {m_{\text{P}}l_{\text{P}}}{t_{\text{P}}^{2}}}={\frac {1}{\varepsilon _{0}}}\ {\frac {q_{\text{P}}^{2}}{l_{\text{P}}^{2}}}}$ (Lorentz–Heaviside version)
${\displaystyle F_{\text{P}}={\frac {m_{\text{P}}l_{\text{P}}}{t_{\text{P}}^{2}}}={\frac {1}{4\pi \varepsilon _{0}}}\ {\frac {q_{\text{P}}^{2}}{l_{\text{P}}^{2}}}}$ (Gaussian version)
${\displaystyle E_{\text{P}}={\frac {m_{\text{P}}l_{\text{P}}^{2}}{t_{\text{P}}^{2}}}=k_{\text{B}}\ T_{\text{P}}.}$

Solving the five equations above for the five unknowns results in a unique set of values for the five base Planck units:

Table 2: Base Planck units
Quantity Expression Metric value Name
Lorentz–Heaviside version Gaussian version Lorentz–Heaviside version Gaussian version
Length (L) ${\displaystyle l_{\text{P}}={\sqrt {\frac {4\pi \hbar G}{c^{3}}}}}$ ${\displaystyle l_{\text{P}}={\sqrt {\frac {\hbar G}{c^{3}}}}}$ 5.729×10−35 m 1.616×10−35 m Planck length
Mass (M) ${\displaystyle m_{\text{P}}={\sqrt {\frac {\hbar c}{4\pi G}}}}$ ${\displaystyle m_{\text{P}}={\sqrt {\frac {\hbar c}{G}}}}$ 6.140×10−9 kg 2.176×10−8 kg Planck mass
Time (T) ${\displaystyle t_{\text{P}}={\sqrt {\frac {4\pi \hbar G}{c^{5}}}}}$ ${\displaystyle t_{\text{P}}={\sqrt {\frac {\hbar G}{c^{5}}}}}$ 1.911×10−43 s 5.391×10−44 s Planck time
Charge (Q) ${\displaystyle q_{\text{P}}={\sqrt {\hbar c\epsilon _{0}}}}$ ${\displaystyle q_{\text{P}}={\sqrt {4\pi \hbar c\epsilon _{0}}}}$ 5.291×10−19 C 1.876×10−18 C Planck charge
Temperature (Θ) ${\displaystyle T_{\text{P}}={\sqrt {\frac {\hbar c^{5}}{4\pi G{k_{\text{B}}}^{2}}}}}$ ${\displaystyle T_{\text{P}}={\sqrt {\frac {\hbar c^{5}}{G{k_{\text{B}}}^{2}}}}}$ 3.997×1031 K 1.417×1032 K Planck temperature

Table 2 clearly defines Planck units in terms of the fundamental constants. Yet relative to other units of measurement such as SI, the values of the Planck units, other than the Planck charge, are only known approximately. This is due to uncertainty in the value of the gravitational constant G as measured relative to SI unit definitions.

Today the value of the speed of light c in SI units is not subject to measurement error, because the SI base unit of length, the metre, is now defined as the length of the path travelled by light in vacuum during a time interval of 1/299792458 of a second. Hence the value of c is now exact by definition, and contributes no uncertainty to the SI equivalents of the Planck units. The same is true of the value of the vacuum permittivity ε0, due to the definition of ampere which sets the vacuum permeability μ0 to 4π × 10−7 H/m and the fact that μ0ε0 = 1/c2. The numerical value of the reduced Planck constant ħ has been determined experimentally to 12 parts per billion, while that of G has been determined experimentally to no better than 1 part in 21300 (or 47000 parts per billion).[2] G appears in the definition of almost every Planck unit in Tables 2 and 3, but not all. Hence the uncertainty in the values of the Table 2 and 3 SI equivalents of the Planck units derives almost entirely from uncertainty in the value of G. (The propagation of the error in G is a function of the exponent of G in the algebraic expression for a unit. Since that exponent is ±1/2 for every base unit other than Planck charge, the relative uncertainty of each base unit is about one half that of G. This is indeed the case; according to CODATA, the experimental values of the SI equivalents of the base Planck units are known to about 1 part in 43500, or 23000 parts per billion.)

## Derived units

In any system of measurement, units for many physical quantities can be derived from base units. Table 3 offers a sample of derived Planck units, some of which in fact are seldom used. As with the base units, their use is mostly confined to theoretical physics because most of them are too large or too small for empirical or practical use and there are large uncertainties in their values.

Table 3: Derived Planck units
Name Dimension Expression Approximate SI equivalent
Lorentz–Heaviside version Gaussian version Lorentz–Heaviside version Gaussian version
Planck area area (L2) ${\displaystyle A_{\text{P}}=l_{\text{P}}^{2}={\frac {4\pi \hbar G}{c^{3}}}}$ ${\displaystyle A_{\text{P}}=l_{\text{P}}^{2}={\frac {\hbar G}{c^{3}}}}$ 3.2826×10−69 m2 2.6122×10−70 m2
Planck volume volume (L3) ${\displaystyle V_{\text{P}}=l_{\text{P}}^{3}={\sqrt {\frac {64\pi ^{3}\hbar ^{3}G^{3}}{c^{9}}}}}$ ${\displaystyle V_{\text{P}}=l_{\text{P}}^{3}={\sqrt {\frac {\hbar ^{3}G^{3}}{c^{9}}}}}$ 1.8807×10−103 m3 4.2219×10−105 m3
Planck speed speed (LT−1) ${\displaystyle v_{\text{P}}={\frac {l_{\text{P}}}{t_{\text{P}}}}=c}$ 2.99792×108 m/s
Planck acceleration acceleration (LT−2) ${\displaystyle a_{\text{P}}={\frac {v_{\text{P}}}{t_{\text{P}}}}={\sqrt {\frac {c^{7}}{4\pi \hbar G}}}}$ ${\displaystyle a_{\text{P}}={\frac {v_{\text{P}}}{t_{\text{P}}}}={\sqrt {\frac {c^{7}}{\hbar G}}}}$ 1.568677×1051 m/s2 5.560817×1051 m/s2
Planck momentum momentum (LMT−1) ${\displaystyle p_{\text{P}}=m_{\text{P}}v_{\text{P}}={\frac {\hbar }{l_{\text{P}}}}={\sqrt {\frac {\hbar c^{3}}{4\pi G}}}}$ ${\displaystyle p_{\text{P}}=m_{\text{P}}v_{\text{P}}={\frac {\hbar }{l_{\text{P}}}}={\sqrt {\frac {\hbar c^{3}}{G}}}}$ 1.84064 kg⋅m/s 6.52489 kg⋅m/s
Planck force force (LMT−2) ${\displaystyle F_{\text{P}}=m_{\text{P}}a_{\text{P}}={\frac {\hbar }{l_{\text{P}}t_{\text{P}}}}={\frac {c^{4}}{4\pi G}}}$ ${\displaystyle F_{\text{P}}=m_{\text{P}}a_{\text{P}}={\frac {\hbar }{l_{\text{P}}t_{\text{P}}}}={\frac {c^{4}}{G}}}$ 9.63122×1042 N 1.21029×1044 N
Planck energy energy (L2MT−2) ${\displaystyle E_{\text{P}}=m_{\text{P}}v_{\text{P}}^{2}={\frac {\hbar }{t_{\text{P}}}}={\sqrt {\frac {\hbar c^{5}}{4\pi G}}}}$ ${\displaystyle E_{\text{P}}=m_{\text{P}}v_{\text{P}}^{2}={\frac {\hbar }{t_{\text{P}}}}={\sqrt {\frac {\hbar c^{5}}{G}}}}$ 5.5181×108 J 1.9561×109 J
Planck power power (L2MT−3) ${\displaystyle P_{\text{P}}={\frac {E_{\text{P}}}{t_{\text{P}}}}={\frac {\hbar }{t_{\text{P}}^{2}}}={\frac {c^{5}}{4\pi G}}}$ ${\displaystyle P_{\text{P}}={\frac {E_{\text{P}}}{t_{\text{P}}}}={\frac {\hbar }{t_{\text{P}}^{2}}}={\frac {c^{5}}{G}}}$ 2.88737×1051 W 3.62837×1052 W
Planck gravitational induction gravitational field (LT−2) ${\displaystyle g_{\text{P}}={\frac {F_{\text{P}}}{m_{\text{P}}}}={\sqrt {\frac {c^{7}}{4\pi \hbar G}}}}$ ${\displaystyle g_{\text{P}}={\frac {F_{\text{P}}}{m_{\text{P}}}}={\sqrt {\frac {c^{7}}{\hbar G}}}}$ 1.568677×1051 m/s2 5.560817×1051 m/s2
Planck specific energy specific energy (L2T−2) ${\displaystyle h_{\text{P}}={\frac {E_{\text{P}}}{m_{\text{P}}}}=c^{2}}$ 8.98755×1016 m2/s2
Planck angle angle (LL−1) ${\displaystyle \theta _{\text{P}}={\frac {l_{\text{P}}}{l_{\text{P}}}}=1}$ 1 rad
Planck angular frequency angular frequency (T−1) ${\displaystyle \omega _{\text{P}}={\frac {\theta _{\text{P}}}{t_{\text{P}}}}={\sqrt {\frac {c^{5}}{4\pi \hbar G}}}}$ ${\displaystyle \omega _{\text{P}}={\frac {\theta _{\text{P}}}{t_{\text{P}}}}={\sqrt {\frac {c^{5}}{\hbar G}}}}$ 5.23254×1042 rad/s 1.85489×1043 rad/s
Planck angular acceleration angular acceleration (T−2) ${\displaystyle \alpha _{\text{P}}={\frac {\omega _{\text{P}}}{t_{\text{P}}}}={\frac {c^{5}}{4\pi \hbar G}}}$ ${\displaystyle \alpha _{\text{P}}={\frac {\omega _{\text{P}}}{t_{\text{P}}}}={\frac {c^{5}}{\hbar G}}}$ 2.73795×1085 rad/s2 3.44061×1086 rad/s2
Planck rotational inertia rotational inertia (L2M) ${\displaystyle I_{\text{P}}=m_{\text{P}}l_{\text{P}}^{2}={\sqrt {\frac {4\pi \hbar ^{2}G}{c^{5}}}}}$ ${\displaystyle I_{\text{P}}=m_{\text{P}}l_{\text{P}}^{2}={\sqrt {\frac {\hbar ^{2}G}{c^{5}}}}}$ 1.96257×10−60 kg⋅m2 5.53631×10−61 kg⋅m2
Planck angular momentum angular momentum (L2MT−1) ${\displaystyle L_{\text{P}}=I_{\text{P}}\omega _{\text{P}}=l_{\text{P}}p_{\text{P}}=\hbar }$ 1.05457×10−34 J⋅s
Planck torque torque (L2MT−2) ${\displaystyle \tau _{\text{P}}=F_{\text{P}}l_{\text{P}}={\frac {\hbar }{t_{\text{P}}}}={\sqrt {\frac {\hbar c^{5}}{4\pi G}}}}$ ${\displaystyle \tau _{\text{P}}=F_{\text{P}}l_{\text{P}}={\frac {\hbar }{t_{\text{P}}}}={\sqrt {\frac {\hbar c^{5}}{G}}}}$ 5.5181×108 N⋅m 1.9561×109 N⋅m
Planck solid angle solid angle (L2L−2) ${\displaystyle \Omega _{\text{P}}=\theta _{\text{P}}^{2}={\frac {l_{\text{P}}^{2}}{l_{\text{P}}^{2}}}=1}$ 1 sr
Planck density density (L−3M) ${\displaystyle d_{\text{P}}={\frac {m_{\text{P}}}{V_{\text{P}}}}={\frac {\hbar t_{\text{P}}}{l_{\text{P}}^{5}}}={\frac {c^{5}}{16\pi ^{2}\hbar G^{2}}}}$ ${\displaystyle d_{\text{P}}={\frac {m_{\text{P}}}{V_{\text{P}}}}={\frac {\hbar t_{\text{P}}}{l_{\text{P}}^{5}}}={\frac {c^{5}}{\hbar G^{2}}}}$ 3.26456×1094 kg/m3 5.15518×1096 kg/m3
Planck energy density energy density (L−1MT−2) ${\displaystyle \rho _{\text{P}}={\frac {E_{\text{P}}}{V_{\text{P}}}}={\frac {c^{7}}{16\pi ^{2}\hbar G^{2}}}}$ ${\displaystyle \rho _{\text{P}}={\frac {E_{\text{P}}}{V_{\text{P}}}}={\frac {c^{7}}{\hbar G^{2}}}}$ 2.934×10111 J/m3 4.633×10113 J/m3
Planck intensity intensity (MT−3) ${\displaystyle I_{\text{P}}={\frac {P_{\text{P}}}{l_{\text{P}}^{2}}}={\frac {c^{8}}{16\pi ^{2}\hbar G^{2}}}}$ ${\displaystyle I_{\text{P}}={\frac {P_{\text{P}}}{l_{\text{P}}^{2}}}={\frac {c^{8}}{\hbar G^{2}}}}$ 8.79603×10119 W/m2 1.38901×10122 W/m2
Planck radiant intensity radiant intensity (L2MT−3) ${\displaystyle I_{\text{P}}={\frac {P_{\text{P}}}{\Omega _{\text{P}}}}={\frac {c^{5}}{4\pi G}}}$ ${\displaystyle I_{\text{P}}={\frac {P_{\text{P}}}{\Omega _{\text{P}}}}={\frac {c^{5}}{G}}}$ 2.88737×1051 W/sr 3.62837×1052 W/sr
Planck pressure pressure (L−1MT−2) ${\displaystyle P_{\text{P}}={\frac {F_{\text{P}}}{A_{\text{P}}}}={\frac {\hbar }{l_{\text{P}}^{3}t_{\text{P}}}}={\frac {c^{7}}{16\pi ^{2}\hbar G^{2}}}}$ ${\displaystyle P_{\text{P}}={\frac {F_{\text{P}}}{A_{\text{P}}}}={\frac {\hbar }{l_{\text{P}}^{3}t_{\text{P}}}}={\frac {c^{7}}{\hbar G^{2}}}}$ 2.934×10111 Pa 4.633×10113 Pa
Planck volumetric flow rate volumetric flow rate (L3T−1) ${\displaystyle Q_{\text{P}}={\frac {V_{\text{P}}}{t_{\text{P}}}}=l_{\text{P}}^{2}v_{\text{P}}={\frac {4\pi \hbar G}{c^{2}}}}$ ${\displaystyle Q_{\text{P}}={\frac {V_{\text{P}}}{t_{\text{P}}}}=l_{\text{P}}^{2}v_{\text{P}}={\frac {\hbar G}{c^{2}}}}$ 9.84×10−61 m3/s 7.83×10−62 m3/s
Planck viscosity viscosity (L−1MT−1) ${\displaystyle \mu _{\text{P}}=P_{\text{P}}t_{\text{P}}={\sqrt {\frac {c^{9}}{64\pi ^{3}G^{3}\hbar }}}}$ ${\displaystyle \mu _{\text{P}}=P_{\text{P}}t_{\text{P}}={\sqrt {\frac {c^{9}}{G^{3}\hbar }}}}$ 5.607×1068 Pa⋅s 2.498×1070 Pa⋅s
Planck current current (T−1Q) ${\displaystyle I_{\text{P}}={\frac {q_{\text{P}}}{t_{\text{P}}}}={\sqrt {\frac {\epsilon _{0}c^{6}}{4\pi G}}}}$ ${\displaystyle I_{\text{P}}={\frac {q_{\text{P}}}{t_{\text{P}}}}={\sqrt {\frac {4\pi \epsilon _{0}c^{6}}{G}}}}$ 2.7684×1024 A 3.4789×1025 A
Planck voltage voltage (L2MT−2Q−1) ${\displaystyle V_{\text{P}}={\frac {E_{\text{P}}}{q_{\text{P}}}}={\frac {\hbar }{t_{\text{P}}q_{\text{P}}}}={\sqrt {\frac {c^{4}}{4\pi \epsilon _{0}G}}}}$ 1.04296×1027 V
Planck impedance resistance (L2MT−1Q−2) ${\displaystyle Z_{\text{P}}={\frac {V_{\text{P}}}{I_{\text{P}}}}={\frac {\hbar }{q_{\text{P}}^{2}}}={\frac {1}{\epsilon _{0}c}}=Z_{0}}$ ${\displaystyle Z_{\text{P}}={\frac {V_{\text{P}}}{I_{\text{P}}}}={\frac {\hbar }{q_{\text{P}}^{2}}}={\frac {1}{4\pi \epsilon _{0}c}}={\frac {Z_{0}}{4\pi }}}$ 376.7303135 Ω 29.9792458 Ω
Planck capacitance capacitance (L−2M−1T2Q2) ${\displaystyle C_{\text{P}}={\frac {q_{\text{P}}}{V_{\text{P}}}}={\frac {t_{\text{P}}q_{\text{P}}^{2}}{\hbar }}={\sqrt {\frac {4\pi \epsilon _{0}^{2}G\hbar }{c^{3}}}}}$ ${\displaystyle C_{\text{P}}={\frac {q_{\text{P}}}{V_{\text{P}}}}={\frac {t_{\text{P}}q_{\text{P}}^{2}}{\hbar }}={\sqrt {\frac {16\pi ^{2}\epsilon _{0}^{2}G\hbar }{c^{3}}}}}$ 5.0729×10−46 F 1.7983×10−45 F
Planck inductance inductance (L2MQ−2) ${\displaystyle L_{\text{P}}={\frac {E_{\text{P}}}{I_{\text{P}}}}={\frac {m_{\text{P}}l_{\text{P}}^{2}}{q_{\text{P}}^{2}}}={\sqrt {\frac {4\pi G\hbar }{c^{7}\epsilon _{0}^{2}}}}}$ ${\displaystyle L_{\text{P}}={\frac {E_{\text{P}}}{I_{\text{P}}}}={\frac {m_{\text{P}}l_{\text{P}}^{2}}{q_{\text{P}}^{2}}}={\sqrt {\frac {G\hbar }{c^{7}16\pi ^{2}\epsilon _{0}^{2}}}}}$ 7.200×10−41 H 1.616×10−42 H
Planck electrical conductivity electrical conductivity (L−3M−1TQ2) ${\displaystyle \sigma _{\text{P}}={\frac {1}{Z_{\text{P}}l_{\text{P}}}}={\sqrt {\frac {\epsilon _{0}^{2}c^{5}}{4\pi \hbar G}}}}$ ${\displaystyle \sigma _{\text{P}}={\frac {1}{Z_{\text{P}}l_{\text{P}}}}={\sqrt {\frac {4\pi \epsilon _{0}^{2}c^{5}}{\hbar G}}}}$ 4.63299×1031 S/m 5.82199×1032 S/m
Planck permittivity permittivity (L−3M−1T2Q2) ${\displaystyle \epsilon _{\text{P}}={\frac {C_{\text{P}}}{l_{\text{P}}}}=\epsilon _{0}}$ ${\displaystyle \epsilon _{\text{P}}={\frac {C_{\text{P}}}{l_{\text{P}}}}=4\pi \epsilon _{0}}$ 8.85419×10−12 F/m 1.11265×10−10 F/m
Planck permeability permeability (LMQ−2) ${\displaystyle \mu _{\text{P}}={\frac {L_{\text{P}}}{l_{\text{P}}}}={\frac {1}{\epsilon _{0}c^{2}}}=\mu _{0}}$ ${\displaystyle \mu _{\text{P}}={\frac {L_{\text{P}}}{l_{\text{P}}}}={\frac {1}{4\pi \epsilon _{0}c^{2}}}={\frac {\mu _{0}}{4\pi }}}$ 1.25664×10−6 H/m 1.00000×10−7 H/m
Planck electric induction electric field (LMT−2Q−1) ${\displaystyle E_{\text{P}}={\frac {F_{\text{P}}}{q_{\text{P}}}}={\sqrt {\frac {c^{7}}{16\pi ^{2}\hbar \epsilon _{0}G^{2}}}}}$ ${\displaystyle E_{\text{P}}={\frac {F_{\text{P}}}{q_{\text{P}}}}={\sqrt {\frac {c^{7}}{4\pi \hbar \epsilon _{0}G^{2}}}}}$ 1.8204×1061 V/m 6.4530×1061 V/m
Planck magnetic induction magnetic field (MT−1Q−1) ${\displaystyle B_{\text{P}}={\frac {F_{\text{P}}}{l_{\text{P}}I_{\text{P}}}}={\sqrt {\frac {c^{5}}{16\pi ^{2}\hbar \epsilon _{0}G^{2}}}}}$ ${\displaystyle B_{\text{P}}={\frac {F_{\text{P}}}{l_{\text{P}}I_{\text{P}}}}={\sqrt {\frac {c^{5}}{4\pi \hbar \epsilon _{0}G^{2}}}}}$ 6.0721×1052 T 2.1525×1053 T
Planck electric flux electric flux (L3MT−2Q−1) ${\displaystyle \Phi _{E{\text{P}}}=E_{\text{P}}A_{\text{P}}={\sqrt {\frac {c\hbar }{\epsilon _{0}}}}}$ ${\displaystyle \Phi _{E{\text{P}}}=E_{\text{P}}A_{\text{P}}={\sqrt {\frac {c\hbar }{4\pi \epsilon _{0}}}}}$ 5.97550×10−8 V⋅m 1.68566×10−8 V⋅m
Planck magnetic flux magnetic flux (L2MT−1Q−1) ${\displaystyle \Phi _{B{\text{P}}}=B_{\text{P}}A_{\text{P}}={\sqrt {\frac {\hbar }{c\epsilon _{0}}}}}$ ${\displaystyle \Phi _{B{\text{P}}}=B_{\text{P}}A_{\text{P}}={\sqrt {\frac {\hbar }{4\pi c\epsilon _{0}}}}}$ 1.99321×10−16 T⋅m2 5.62275×10−17 T⋅m2
Planck entropy entropy (L2MT−2Θ−1) ${\displaystyle S_{\text{P}}={\frac {E_{\text{P}}}{T_{\text{P}}}}=k_{\text{B}}}$ 1.38065×10−23 J/K
Planck specific heat capacity specific heat capacity (L2T−2Θ−1) ${\displaystyle c_{\text{P}}={\frac {E_{\text{P}}}{m_{\text{P}}T_{\text{P}}}}={\frac {k_{\text{B}}}{m_{\text{P}}}}={\sqrt {\frac {4\pi Gk_{\text{B}}^{2}}{c\hbar }}}}$ ${\displaystyle c_{\text{P}}={\frac {E_{\text{P}}}{m_{\text{P}}T_{\text{P}}}}={\frac {k_{\text{B}}}{m_{\text{P}}}}={\sqrt {\frac {Gk_{\text{B}}^{2}}{c\hbar }}}}$ 2.24872×10−15 J/kg⋅K 6.34352×10−16 J/kg⋅K
Planck thermal conductivity thermal conductivity (LMT−3Θ−1) ${\displaystyle \lambda _{\text{P}}={\frac {P_{\text{P}}}{l_{\text{P}}T_{\text{P}}}}={\sqrt {\frac {c^{8}k_{\text{B}}^{2}}{4\pi \hbar ^{2}G}}}}$ ${\displaystyle \lambda _{\text{P}}={\frac {P_{\text{P}}}{l_{\text{P}}T_{\text{P}}}}={\sqrt {\frac {c^{8}k_{\text{B}}^{2}}{\hbar ^{2}G}}}}$ 3.65165×1049 W/m⋅K 1.29448×1050 W/m⋅K

The charge, as other Planck units, was not originally defined by Planck. It is a unit of charge that is a natural addition to the other units of Planck, and is used in some publications.[6][7] The elementary charge ${\displaystyle e}$, measured in terms of the Planck charge, is

${\displaystyle e={\sqrt {4\pi \alpha }}\cdot q_{\text{P}}\approx 0.302822121\cdot q_{\text{P}}\,}$ (Lorentz–Heaviside version)
${\displaystyle e={\sqrt {\alpha }}\cdot q_{\text{P}}\approx 0.085424543\cdot q_{\text{P}}\,}$ (Gaussian version)

where ${\displaystyle {\alpha }}$ is the fine-structure constant

${\displaystyle \alpha ={\frac {k_{e}e^{2}}{\hbar c}}\approx {\frac {1}{137.03599911}}}$
${\displaystyle \alpha ={\frac {1}{4\pi }}\left({\frac {e}{q_{\text{P}}}}\right)^{2}}$ (Lorentz–Heaviside version)
${\displaystyle \alpha =\left({\frac {e}{q_{\text{P}}}}\right)^{2}}$ (Gaussian version)

The fine-structure constant ${\displaystyle \alpha }$ is also called the electromagnetic coupling constant, thus comparing with the gravitational coupling constant ${\displaystyle \alpha _{G}}$. The electron rest mass ${\displaystyle m_{e}}$ measured in terms of the Planck mass, is

${\displaystyle m_{e}={\sqrt {4\pi \alpha _{G}}}\cdot m_{\text{P}}\approx 1.48368\times 10^{-22}\cdot m_{\text{P}}\,}$ (Lorentz–Heaviside version)
${\displaystyle m_{e}={\sqrt {\alpha _{G}}}\cdot m_{\text{P}}\approx 4.18539\times 10^{-23}\cdot m_{\text{P}}\,}$ (Gaussian version)

where ${\displaystyle {\alpha _{G}}}$ is the gravitational coupling constant

${\displaystyle \alpha _{G}={\frac {Gm_{e}^{2}}{\hbar c}}\approx 1.5718\times 10^{-45}}$
${\displaystyle \alpha _{G}={\frac {1}{4\pi }}\left({\frac {m_{e}}{m_{\text{P}}}}\right)^{2}}$ (Lorentz–Heaviside version)
${\displaystyle \alpha _{G}=\left({\frac {m_{e}}{m_{\text{P}}}}\right)^{2}}$ (Gaussian version)

Some Planck units are suitable for measuring quantities that are familiar from daily experience. For example:

However, most Planck units are many orders of magnitude too large or too small to be of practical use, so that Planck units as a system are really only relevant to theoretical physics. In fact, 1 Planck unit is often the largest or smallest value of a physical quantity that makes sense according to our current understanding. For example:

• 1 Planck speed is the speed of light in a vacuum, the maximum possible physical speed in special relativity;[8] 1 nano-Planck speed is about 1.079 km/h.
• Our understanding of the Big Bang begins with the Planck epoch, when the universe was 1 Planck time old and 1 Planck length in diameter, and had a Planck temperature of 1. At that moment, quantum theory as presently understood becomes applicable. Understanding the universe when it was less than 1 Planck time old requires a theory of quantum gravity that would incorporate quantum effects into general relativity. Such a theory does not yet exist.

## Significance

Planck units are free of anthropocentric arbitrariness. Some physicists argue that communication with extraterrestrial intelligence would have to employ such a system of units in order to be understood.[9] Unlike the metre and second, which exist as base units in the SI system for historical reasons, the Planck length and Planck time are conceptually linked at a fundamental physical level.

Natural units help physicists to reframe questions. Frank Wilczek puts it succinctly:

We see that the question [posed] is not, "Why is gravity so feeble?" but rather, "Why is the proton's mass so small?" For in natural (Planck) units, the strength of gravity simply is what it is, a primary quantity, while the proton's mass is the tiny number [1/(13 quintillion)].[10]

While it is true that the electrostatic repulsive force between two protons (alone in free space) greatly exceeds the gravitational attractive force between the same two protons, this is not about the relative strengths of the two fundamental forces. From the point of view of Planck units, this is comparing apples to oranges, because mass and electric charge are incommensurable quantities. Rather, the disparity of magnitude of force is a manifestation of the fact that the charge on the protons is approximately the unit charge but the mass of the protons is far less than the unit mass.

### Cosmology

In Big Bang cosmology, the Planck epoch or Planck era is the earliest stage of the Big Bang, before the time passed was equal to the Planck time, tP, or approximately 10−43 seconds.[11] There is no currently available physical theory to describe such short times, and it is not clear in what sense the concept of time is meaningful for values smaller than the Planck time. It is generally assumed that quantum effects of gravity dominate physical interactions at this time scale. At this scale, the unified force of the Standard Model is assumed to be unified with gravitation. Immeasurably hot and dense, the state of the Planck epoch was succeeded by the grand unification epoch, where gravitation is separated from the unified force of the Standard Model, in turn followed by the inflationary epoch, which ended after about 10−32 seconds (or about 1010 tP).[12]

Relative to the Planck epoch, the observable universe today looks extreme when expressed in Planck units, as in this set of approximations:[13][14]

Table 4: Today's universe in Planck units.
Property of
present-day Observable Universe
Approximate number
of Planck units
Equivalents
Age 8.08 × 1060 tP 4.35 × 1017 s, or 13.8 × 109 years
Diameter 5.4 × 1061 lP 8.7 × 1026 m or 9.2 × 1010 ly
Volume 8.4559 × 10184 VP 3.57 × 1080 m3 or 4.22 × 1032 ly3
Mass approx. 1060 mP 3 × 1052 kg or 1.5 × 1022 solar masses (only counting stars)
1080 protons (sometimes known as the Eddington number)
Density 1.8 × 10−123 dP 9.9 × 10−27 kg m−3
Temperature 1.9 × 10−32 TP 2.725 K
temperature of the cosmic microwave background radiation
Cosmological constant 5.6 × 10−122 t−2
P
1.9 × 10−35 s−2
Hubble constant 1.18 × 10−61 t−1
P
2.2 × 10−18 s−1 or 67.8 (km/s)/Mpc

The recurrence of large numbers close or related to 1060 in the above table is a coincidence that intrigues some theorists. It is an example of the kind of large numbers coincidence that led theorists such as Eddington and Dirac to develop alternative physical theories (e.g. a variable speed of light or Dirac varying-G theory).[15] After the measurement of the cosmological constant in 1998, estimated at 10−122 in Planck units, it was noted that this is suggestively close to the reciprocal of the age of the universe squared.[16] Barrow and Shaw (2011) proposed a modified theory in which Λ is a field evolving in such a way that its value remains Λ ~ T−2 throughout the history of the universe.[17]

## History

Natural units began in 1881, when George Johnstone Stoney, noting that electric charge is quantized, derived units of length, time, and mass, now named Stoney units in his honor, by normalizing G, c, and the electron charge, e, to 1.

Already in 1899 (i.e. one year before the advent of quantum theory) Max Planck introduced what became later known as Planck's constant.[18][19] At the end of the paper, Planck introduced, as a consequence of his discovery, the base units later named in his honor. The Planck units are based on the quantum of action, now usually known as Planck's constant. Planck called the constant b in his paper, though h (or ħ) is now common. However, at that time it was entering Wien's radiation law which Planck thought to be correct. Planck underlined the universality of the new unit system, writing:

...ihre Bedeutung für alle Zeiten und für alle, auch außerirdische und außermenschliche Kulturen notwendig behalten und welche daher als »natürliche Maßeinheiten« bezeichnet werden können...

...These necessarily retain their meaning for all times and for all civilizations, even extraterrestrial and non-human ones, and can therefore be designated as "natural units"...

Planck considered only the units based on the universal constants G, ħ, c, and kB to arrive at natural units for length, time, mass, and temperature.[19] Planck did not adopt any electromagnetic units. However, since the non-rationalized gravitational constant, G, is set to 1, a natural extension of Planck units to a unit of electric charge is to also set the non-rationalized Coulomb constant, ke, to 1 as well (as well as the Stoney units).[20] This is the non-rationalized Planck units (Planck units with the Gaussian version), which is more convenient but not rationalized, there is also a Planck system which is rationalized (Planck units with the Lorentz-Heaviside version), set 4πG and ε0 (instead of G and ke) to 1, which may be less convenient but is rationalized. Another convention is to use the elementary charge as the basic unit of electric charge in the Planck system.[21] Such a system is convenient for black hole physics. The two conventions for unit charge differ by a factor of the square root of the fine-structure constant. Planck's paper also gave numerical values for the base units that were close to modern values.

## List of physical equations

Physical quantities that have different dimensions (such as time and length) cannot be equated even if they are numerically equal (1 second is not the same as 1 metre). In theoretical physics, however, this scruple can be set aside, by a process called nondimensionalization. Table 6 shows how the use of Planck units simplifies many fundamental equations of physics, because this gives each of the five fundamental constants, and products of them, a simple numeric value of 1. In the SI form, the units should be accounted for. In the nondimensionalized form, the units, which are now Planck units, need not be written if their use is understood.

Table 5: How Planck units simplify the key equations of physics
SI form Lorentz-Heaviside version Planck form Gaussian version Planck form
Mass–energy equivalence in special relativity ${\displaystyle {E=mc^{2}}\ }$ ${\displaystyle {E=m}\ }$
Energy–momentum relation ${\displaystyle E^{2}=m^{2}c^{4}+p^{2}c^{2}\;}$ ${\displaystyle E^{2}=m^{2}+p^{2}\;}$
Newton's law of universal gravitation ${\displaystyle F=G{\frac {m_{1}m_{2}}{r^{2}}}}$ ${\displaystyle F={\frac {m_{1}m_{2}}{4\pi r^{2}}}}$ ${\displaystyle F={\frac {m_{1}m_{2}}{r^{2}}}}$
Einstein field equations in general relativity ${\displaystyle {G_{\mu \nu }=8\pi {G \over c^{4}}T_{\mu \nu }}\ }$ ${\displaystyle {G_{\mu \nu }=2T_{\mu \nu }}\ }$ ${\displaystyle {G_{\mu \nu }=8\pi T_{\mu \nu }}\ }$
Planck–Einstein relation for energy and angular frequency ${\displaystyle {E=\hbar \omega }\ }$ ${\displaystyle {E=\omega }\ }$
Heisenberg's uncertainty principle ${\displaystyle \Delta x\cdot \Delta p\geq {\frac {\hbar }{2}}}$ ${\displaystyle \Delta x\cdot \Delta p\geq {\frac {1}{2}}}$
Schrödinger's equation ${\displaystyle -{\frac {\hbar ^{2}}{2m}}\nabla ^{2}\psi (\mathbf {r} ,t)+V(\mathbf {r} ,t)\psi (\mathbf {r} ,t)=i\hbar {\frac {\partial \psi (\mathbf {r} ,t)}{\partial t}}}$ ${\displaystyle -{\frac {1}{2m}}\nabla ^{2}\psi (\mathbf {r} ,t)+V(\mathbf {r} ,t)\psi (\mathbf {r} ,t)=i{\frac {\partial \psi (\mathbf {r} ,t)}{\partial t}}}$
Hamiltonian form of Schrödinger's equation ${\displaystyle H\left|\psi _{t}\right\rangle =i\hbar {\frac {\partial }{\partial t}}\left|\psi _{t}\right\rangle }$ ${\displaystyle H\left|\psi _{t}\right\rangle =i{\frac {\partial }{\partial t}}\left|\psi _{t}\right\rangle }$
Covariant form of the Dirac equation ${\displaystyle \ (i\hbar \gamma ^{\mu }\partial _{\mu }-mc)\psi =0}$ ${\displaystyle \ (i\gamma ^{\mu }\partial _{\mu }-m)\psi =0}$
The vacuum permeability ${\displaystyle \mu _{0}={\frac {1}{\epsilon _{0}c^{2}}}}$ ${\displaystyle \mu _{0}=1}$ ${\displaystyle \mu _{0}=4\pi }$
The impedance of free space ${\displaystyle Z_{0}={\frac {\mathbf {E} }{\mathbf {H} }}={\sqrt {\frac {\mu _{0}}{\epsilon _{0}}}}={\frac {1}{\epsilon _{0}c}}=\mu _{0}c}$ ${\displaystyle Z_{0}=1}$ ${\displaystyle Z_{0}=4\pi }$
Coulomb's law ${\displaystyle F={\frac {1}{4\pi \epsilon _{0}}}{\frac {q_{1}q_{2}}{r^{2}}}}$ ${\displaystyle F={\frac {q_{1}q_{2}}{4\pi r^{2}}}}$ ${\displaystyle F={\frac {q_{1}q_{2}}{r^{2}}}}$
Biot–Savart law ${\displaystyle \mathbf {B} (\mathbf {r} )={\frac {\mu _{0}}{4\pi }}\int _{C}{\frac {I\,d{\boldsymbol {\ell }}\times \mathbf {r'} }{|\mathbf {r'} |^{3}}}}$ ${\displaystyle \mathbf {B} (\mathbf {r} )={\frac {1}{4\pi }}\int _{C}{\frac {I\,d{\boldsymbol {\ell }}\times \mathbf {r'} }{|\mathbf {r'} |^{3}}}}$ ${\displaystyle \mathbf {B} (\mathbf {r} )=\int _{C}{\frac {I\,d{\boldsymbol {\ell }}\times \mathbf {r'} }{|\mathbf {r'} |^{3}}}}$
Equation of electric fields in free space ${\displaystyle \mathbf {D} =\epsilon _{0}\mathbf {E} }$ ${\displaystyle \mathbf {D} =\mathbf {E} }$ ${\displaystyle \mathbf {D} ={\frac {\mathbf {E} }{4\pi }}}$
Equation of magnetic fields in free space ${\displaystyle \mathbf {H} ={\frac {\mathbf {B} }{\mu _{0}}}}$ ${\displaystyle \mathbf {H} =\mathbf {B} }$ ${\displaystyle \mathbf {H} ={\frac {\mathbf {B} }{4\pi }}}$
Maxwell's equations ${\displaystyle \nabla \cdot \mathbf {E} ={\frac {1}{\epsilon _{0}}}\rho }$

${\displaystyle \nabla \cdot \mathbf {B} =0\ }$
${\displaystyle \nabla \times \mathbf {E} =-{\frac {\partial \mathbf {B} }{\partial t}}}$
${\displaystyle \nabla \times \mathbf {B} ={\frac {1}{c^{2}}}\left({\frac {1}{\epsilon _{0}}}\mathbf {J} +{\frac {\partial \mathbf {E} }{\partial t}}\right)}$

${\displaystyle \nabla \cdot \mathbf {E} =\rho }$

${\displaystyle \nabla \cdot \mathbf {B} =0\ }$
${\displaystyle \nabla \times \mathbf {E} =-{\frac {\partial \mathbf {B} }{\partial t}}}$
${\displaystyle \nabla \times \mathbf {B} =\mathbf {J} +{\frac {\partial \mathbf {E} }{\partial t}}}$

${\displaystyle \nabla \cdot \mathbf {E} =4\pi \rho \ }$

${\displaystyle \nabla \cdot \mathbf {B} =0\ }$
${\displaystyle \nabla \times \mathbf {E} =-{\frac {\partial \mathbf {B} }{\partial t}}}$
${\displaystyle \nabla \times \mathbf {B} =4\pi \mathbf {J} +{\frac {\partial \mathbf {E} }{\partial t}}}$

Josephson constant KJ defined ${\displaystyle K_{J}={\frac {e}{\pi \hbar }}}$ ${\displaystyle K_{J}={\sqrt {\frac {4\alpha }{\pi }}}}$ ${\displaystyle K_{J}={\frac {\sqrt {\alpha }}{\pi }}}$
von Klitzing constant RK defined ${\displaystyle R_{K}={\frac {2\pi \hbar }{e^{2}}}}$ ${\displaystyle R_{K}={\frac {1}{2\alpha }}}$ ${\displaystyle R_{K}={\frac {2\pi }{\alpha }}}$
Ideal gas law ${\displaystyle PV=Nk_{\text{B}}T}$ ${\displaystyle PV=NT}$
Unruh temperature ${\displaystyle T={\frac {\hbar a}{2\pi ck_{B}}}}$ ${\displaystyle T={\frac {a}{2\pi }}}$
Thermal energy per particle per degree of freedom ${\displaystyle {E={\tfrac {1}{2}}k_{\text{B}}T}\ }$ ${\displaystyle {E={\tfrac {1}{2}}T}\ }$
Boltzmann's entropy formula ${\displaystyle {S=k_{\text{B}}\ln \Omega }\ }$ ${\displaystyle {S=\ln \Omega }\ }$
Stefan–Boltzmann constant σ defined ${\displaystyle \sigma ={\frac {\pi ^{2}k_{\text{B}}^{4}}{60\hbar ^{3}c^{2}}}}$ ${\displaystyle \sigma ={\frac {\pi ^{2}}{60}}}$
Planck's law (surface intensity per unit solid angle per unit angular frequency) for black body at temperature T. ${\displaystyle I(\omega ,T)={\frac {\hbar \omega ^{3}}{4\pi ^{3}c^{2}}}~{\frac {1}{e^{\frac {\hbar \omega }{k_{\text{B}}T}}-1}}}$ ${\displaystyle I(\omega ,T)={\frac {\omega ^{3}}{4\pi ^{3}}}~{\frac {1}{e^{\omega /T}-1}}}$
BekensteinHawking black hole entropy[22] ${\displaystyle S_{\text{BH}}={\frac {A_{\text{BH}}k_{\text{B}}c^{3}}{4G\hbar }}={\frac {4\pi Gk_{\text{B}}m_{\text{BH}}^{2}}{\hbar c}}}$ ${\displaystyle S_{\text{BH}}=\pi A_{\text{BH}}=m_{\text{BH}}^{2}}$ ${\displaystyle S_{\text{BH}}={\frac {A_{\text{BH}}}{4}}=4\pi m_{\text{BH}}^{2}}$

Note: For the elementary charge ${\displaystyle e}$:

${\displaystyle e={\sqrt {4\pi \alpha }}}$ (Lorentz–Heaviside version)
${\displaystyle e={\sqrt {\alpha }}}$ (Gaussian version)

where ${\displaystyle \alpha }$ is the fine-structure constant.

## Alternative choices of normalization

As already stated above, Planck units are derived by "normalizing" the numerical values of certain fundamental constants to 1. These normalizations are neither the only ones possible nor necessarily the best. Moreover, the choice of what factors to normalize, among the factors appearing in the fundamental equations of physics, is not evident, and the values of the Planck units are sensitive to this choice.

The factor 4π is ubiquitous in theoretical physics because the surface area of a sphere of radius r is 4πr2. This, along with the concept of flux, are the basis for the inverse-square law, Gauss's law, and the divergence operator applied to flux density. For example, gravitational and electrostatic fields produced by point charges have spherical symmetry (Barrow 2002: 214–15). The 4πr2 appearing in the denominator of Coulomb's law in rationalized form, for example, follows from the flux of an electrostatic field being distributed uniformly on the surface of a sphere. Likewise for Newton's law of universal gravitation. (If space had more than three spatial dimensions, the factor 4π would have to be changed according to the geometry of the sphere in higher dimensions.)

Hence a substantial body of physical theory developed since Planck (1899) suggests normalizing not G but either 4πG (or 8πG or 16πG) to 1. Doing so would introduce a factor of 1/4π (or 1/8π or 1/16π) into the nondimensionalized form of the law of universal gravitation, consistent with the modern rationalized formulation of Coulomb's law in terms of the vacuum permittivity. In fact, alternative normalizations frequently preserve the factor of 1/4π in the nondimensionalized form of Coulomb's law as well, so that the nondimensionalized Maxwell's equations for electromagnetism and gravitoelectromagnetism both take the same form as those for electromagnetism in SI, which do not have any factors of 4π. When this is applied to electromagnetic constants, ε0, this unit system is called "rationalized" Lorentz–Heaviside units. When applied additionally to gravitation and Planck units, these are called rationalized Planck units[23] and are seen in high-energy physics.

The rationalized Planck units are defined so that ${\displaystyle c=4\pi G=\hbar =\epsilon _{0}=k_{\text{B}}=1}$. These are the Planck units based on Lorentz–Heaviside units (instead of on the more conventional Gaussian units) as depicted above.

There are several possible alternative normalizations.

### Gravity

In 1899, Newton's law of universal gravitation was still seen as exact, rather than as a convenient approximation holding for "small" velocities and masses (the approximate nature of Newton's law was shown following the development of general relativity in 1915). Hence Planck normalized to 1 the gravitational constant G in Newton's law. In theories emerging after 1899, G nearly always appears in formulae multiplied by 4π or a small integer multiple thereof. Hence, a choice to be made when designing a system of natural units is which, if any, instances of 4π appearing in the equations of physics are to be eliminated via the normalization.

• Normalizing 4πG to 1: (such as the Lorentz–Heaviside version Planck units)
• Setting 8πG = 1. This would eliminate 8πG from the Einstein field equations, Einstein–Hilbert action, and the Friedmann equations, for gravitation. Planck units modified so that 8πG = 1 are known as reduced Planck units, because the Planck mass is divided by 8π. Also, the Bekenstein–Hawking formula for the entropy of a black hole simplifies to SBH = (mBH)2/2 = 2πABH.
• Setting 16πG = 1. This would eliminate the constant c4/16πG from the Einstein–Hilbert action. The form of the Einstein field equations with cosmological constant Λ becomes Rμν + Λgμν = 1/2(Rgμν + Tμν).

### Electromagnetism

Planck units normalize to 1 the Coulomb force constant ke = 1/4πε0 (as does the cgs system of units). This sets the Planck impedance, ZP equal to Z0/4π, where Z0 is the characteristic impedance of free space.

${\displaystyle e={\sqrt {4\pi \alpha }}\cdot q_{\text{(P)}}\approx 0.30282212\cdot q_{\text{(P)}}\,}$
where ${\displaystyle {\alpha }\ }$ is the fine-structure constant. This convention is seen in high-energy physics.

### Temperature

Planck normalized to 1 the Boltzmann constant kB.

• Normalizing 1/2kB to 1:
• Removes the factor of 1/2 in the nondimensionalized equation for the thermal energy per particle per degree of freedom.
• Introduces a factor of 2 into the nondimensionalized form of Boltzmann's entropy formula.
• Does not affect the value of any of the base or derived Planck units listed in Tables 2 and 3 other than the Planck temperature, Planck entropy, Planck specific heat capacity, and Planck thermal conductivity, which Planck temperature doubles, and the other three become their half.

## Planck units and the invariant scaling of nature

Some theorists (such as Dirac and Milne) have proposed cosmologies that conjecture that physical "constants" might actually change over time (e.g. a variable speed of light or Dirac varying-G theory). Such cosmologies have not gained mainstream acceptance and yet there is still considerable scientific interest in the possibility that physical "constants" might change, although such propositions introduce difficult questions. Perhaps the first question to address is: How would such a change make a noticeable operational difference in physical measurement or, more fundamentally, our perception of reality? If some particular physical constant had changed, how would we notice it, or how would physical reality be different? Which changed constants result in a meaningful and measurable difference in physical reality? If a physical constant that is not dimensionless, such as the speed of light, did in fact change, would we be able to notice it or measure it unambiguously? – a question examined by Michael Duff in his paper "Comment on time-variation of fundamental constants".[24][25]

George Gamow argued in his book Mr Tompkins in Wonderland that a sufficient change in a dimensionful physical constant, such as the speed of light in a vacuum, would result in obvious perceptible changes. But this idea is challenged:

[An] important lesson we learn from the way that pure numbers like α define the world is what it really means for worlds to be different. The pure number we call the fine structure constant and denote by α is a combination of the electron charge, e, the speed of light, c, and Planck's constant, h. At first we might be tempted to think that a world in which the speed of light was slower would be a different world. But this would be a mistake. If c, h, and e were all changed so that the values they have in metric (or any other) units were different when we looked them up in our tables of physical constants, but the value of α remained the same, this new world would be observationally indistinguishable from our world. The only thing that counts in the definition of worlds are the values of the dimensionless constants of Nature. If all masses were doubled in value [including the Planck mass mP ] you cannot tell because all the pure numbers defined by the ratios of any pair of masses are unchanged.

— Barrow 2002[13]

Referring to Duff's "Comment on time-variation of fundamental constants"[24] and Duff, Okun, and Veneziano's paper "Trialogue on the number of fundamental constants",[26] particularly the section entitled "The operationally indistinguishable world of Mr. Tompkins", if all physical quantities (masses and other properties of particles) were expressed in terms of Planck units, those quantities would be dimensionless numbers (mass divided by the Planck mass, length divided by the Planck length, etc.) and the only quantities that we ultimately measure in physical experiments or in our perception of reality are dimensionless numbers. When one commonly measures a length with a ruler or tape-measure, that person is actually counting tick marks on a given standard or is measuring the length relative to that given standard, which is a dimensionless value. It is no different for physical experiments, as all physical quantities are measured relative to some other like-dimensioned quantity.

We can notice a difference if some dimensionless physical quantity such as fine-structure constant, α, changes or the proton-to-electron mass ratio, mp/me, changes (atomic structures would change) but if all dimensionless physical quantities remained unchanged (this includes all possible ratios of identically dimensioned physical quantity), we cannot tell if a dimensionful quantity, such as the speed of light, c, has changed. And, indeed, the Tompkins concept becomes meaningless in our perception of reality if a dimensional quantity such as c has changed, even drastically.

If the speed of light c, were somehow suddenly cut in half and changed to 1/2c (but with the axiom that all dimensionless physical quantities remain the same), then the Planck length would increase by a factor of 22 from the point of view of some unaffected observer on the outside. Measured by "mortal" observers in terms of Planck units, the new speed of light would remain as 1 new Planck length per 1 new Planck time – which is no different from the old measurement. But, since by axiom, the size of atoms (approximately the Bohr radius) are related to the Planck length by an unchanging dimensionless constant of proportionality:

${\displaystyle a_{0}={\frac {4\pi \epsilon _{0}\hbar ^{2}}{m_{e}e^{2}}}={\frac {m_{\text{P}}}{m_{e}\alpha }}l_{\text{P}}.}$

Then atoms would be bigger (in one dimension) by 22, each of us would be taller by 22, and so would our metre sticks be taller (and wider and thicker) by a factor of 22. Our perception of distance and lengths relative to the Planck length is, by axiom, an unchanging dimensionless constant.

Our clocks would tick slower by a factor of 42 (from the point of view of this unaffected observer on the outside) because the Planck time has increased by 42 but we would not know the difference (our perception of durations of time relative to the Planck time is, by axiom, an unchanging dimensionless constant). This hypothetical unaffected observer on the outside might observe that light now propagates at half the speed that it previously did (as well as all other observed velocities) but it would still travel 299792458 of our new metres in the time elapsed by one of our new seconds (1/2c × 42 ÷ 22 continues to equal 299792458 m/s). We would not notice any difference.

This contradicts what George Gamow writes in his book Mr. Tompkins; there, Gamow suggests that if a dimension-dependent universal constant such as c changed significantly, we would easily notice the difference. The disagreement is better thought of as the ambiguity in the phrase "changing a physical constant"; what would happen depends on whether (1) all other dimensionless constants were kept the same, or whether (2) all other dimension-dependent constants are kept the same. The second choice is a somewhat confusing possibility, since most of our units of measurement are defined in relation to the outcomes of physical experiments, and the experimental results depend on the constants. Gamow does not address this subtlety; the thought experiments he conducts in his popular works assume the second choice for "changing a physical constant". And Duff or Barrow would point out that ascribing a change in measurable reality, i.e. α, to a specific dimensional component quantity, such as c, is unjustified. The very same operational difference in measurement or perceived reality could just as well be caused by a change in h or e if α is changed and no other dimensionless constants are changed. It is only the dimensionless physical constants that ultimately matter in the definition of worlds.[24][27]

This unvarying aspect of the Planck-relative scale, or that of any other system of natural units, leads many theorists to conclude that a hypothetical change in dimensionful physical constants can only be manifest as a change in dimensionless physical constants. One such dimensionless physical constant is the fine-structure constant. There are some experimental physicists who assert they have in fact measured a change in the fine structure constant[28] and this has intensified the debate about the measurement of physical constants. According to some theorists[29] there are some very special circumstances in which changes in the fine-structure constant can be measured as a change in dimensionful physical constants. Others however reject the possibility of measuring a change in dimensionful physical constants under any circumstance.[24] The difficulty or even the impossibility of measuring changes in dimensionful physical constants has led some theorists to debate with each other whether or not a dimensionful physical constant has any practical significance at all and that in turn leads to questions about which dimensionful physical constants are meaningful.[26]

## Notes

1. ^ General relativity predicts that gravitational radiation propagates at the same speed as electromagnetic radiation.

## References

### Citations

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2. ^ a b "Fundamental Physical Constants from NIST". physics.nist.gov.
3. ^ "2018 CODATA Value: Newtonian constant of gravitation". The NIST Reference on Constants, Units, and Uncertainty. NIST. 20 May 2019. Retrieved 20 May 2019.
4. ^ "2018 CODATA Value: reduced Planck constant". The NIST Reference on Constants, Units, and Uncertainty. NIST. 20 May 2019. Retrieved 28 August 2019.
5. ^ "2018 CODATA Value: Boltzmann constant". The NIST Reference on Constants, Units, and Uncertainty. NIST. 20 May 2019. Retrieved 20 May 2019.
6. ^ [Theory of Quantized Space – Date of registration 21/9/1994 N. 344146 protocol 4646 Presidency of the Council of Ministers – Italy – Dep. Information and Publishing, literary, artistic and scientific property]
7. ^
8. ^ Feynman, R. P.; Leighton, R. B.; Sands, M. (1963). "The Special Theory of Relativity". The Feynman Lectures on Physics. 1 "Mainly mechanics, radiation, and heat". Addison-Wesley. pp. 15–9. ISBN 978-0-7382-0008-8. LCCN 63020717.
9. ^ Michael W. Busch, Rachel M. Reddick (2010) "Testing SETI Message Designs," Astrobiology Science Conference 2010, 26–29 April 2010, League City, Texas.
10. ^ Wilczek, Frank (2001). "Scaling Mount Planck I: A View from the Bottom". Physics Today. 54 (6): 12–13. Bibcode:2001PhT....54f..12W. doi:10.1063/1.1387576.
11. ^ Staff. "Birth of the Universe". University of Oregon. Retrieved 24 September 2016. - discusses "Planck time" and "Planck era" at the very beginning of the Universe
12. ^ Edward W. Kolb; Michael S. Turner (1994). The Early Universe. Basic Books. p. 447. ISBN 978-0-201-62674-2. Retrieved 10 April 2010.
13. ^ a b John D. Barrow, 2002. The Constants of Nature; From Alpha to Omega – The Numbers that Encode the Deepest Secrets of the Universe. Pantheon Books. ISBN 0-375-42221-8.
14. ^
15. ^ P.A.M. Dirac (1938). "A New Basis for Cosmology". Proceedings of the Royal Society A. 165 (921): 199–208. Bibcode:1938RSPSA.165..199D. doi:10.1098/rspa.1938.0053.
16. ^ J.D. Barrow and F.J. Tipler, The Anthropic Cosmological Principle, Oxford UP, Oxford (1986), chapter 6.9.
17. ^ Barrow, John D.; Shaw, Douglas J. (2011). "The value of the cosmological constant". General Relativity and Gravitation. 43 (10): 2555–2560. arXiv:1105.3105. Bibcode:2011GReGr..43.2555B. doi:10.1007/s10714-011-1199-1.
18. ^ Planck (1899), p. 479.
19. ^ a b *Tomilin, K. A., 1999, "Natural Systems of Units: To the Centenary Anniversary of the Planck System", 287–296.
20. ^ Pavšic, Matej (2001). The Landscape of Theoretical Physics: A Global View. Fundamental Theories of Physics. 119. Dordrecht: Kluwer Academic. pp. 347–352. arXiv:gr-qc/0610061. doi:10.1007/0-306-47136-1. ISBN 978-0-7923-7006-2.
21. ^ Tomilin, K. (1999). "Fine-structure constant and dimension analysis". Eur. J. Phys. 20 (5): L39–L40. Bibcode:1999EJPh...20L..39T. doi:10.1088/0143-0807/20/5/404.
22. ^ Also see Roger Penrose (1989) The Road to Reality. Oxford Univ. Press: 714-17. Knopf.
23. ^ Sorkin, Rafael (1983). "Kaluza-Klein Monopole". Physical Review Letters. 51 (2): 87–90. Bibcode:1983PhRvL..51...87S. doi:10.1103/PhysRevLett.51.87.
24. ^ a b c d Michael Duff (2002). "Comment on time-variation of fundamental constants". arXiv:hep-th/0208093.
25. ^ Michael Duff (2014). How fundamental are fundamental constants?. arXiv:1412.2040. doi:10.1080/00107514.2014.980093 (inactive 22 January 2020).
26. ^ a b Duff, Michael; Okun, Lev; Veneziano, Gabriele (2002). "Trialogue on the number of fundamental constants". Journal of High Energy Physics. 2002 (3): 023. arXiv:physics/0110060. Bibcode:2002JHEP...03..023D. doi:10.1088/1126-6708/2002/03/023.
27. ^
28. ^ Webb, J. K.; et al. (2001). "Further evidence for cosmological evolution of the fine structure constant". Phys. Rev. Lett. 87 (9): 884. arXiv:astro-ph/0012539v3. Bibcode:2001PhRvL..87i1301W. doi:10.1103/PhysRevLett.87.091301. PMID 11531558.
29. ^ Davies, Paul C.; Davis, T. M.; Lineweaver, C. H. (2002). "Cosmology: Black Holes Constrain Varying Constants". Nature. 418 (6898): 602–3. Bibcode:2002Natur.418..602D. doi:10.1038/418602a. PMID 12167848.