Data:CODATA Recommended Values of the Fundamental Physical Constants 1973

Further information: CODATA Recommended Values of the Fundamental Physical Constants

Quantity	Symbol	Value	ur
Permeability of vacuum (magnetic constant)	μ0	4π × 10−7 H m−1 ≈ 1.256 637 061… × 10−6 H m−1	exact
Speed of light in vacuum	c0	2.997 924 58(1.2) × 108 m s−1	4 × 10−9
Permittivity of vacuum (electric constant)	ε0 = (μ0c20)−1	8.854 187 82(7) × 10−12 F m−1	8 × 10−9
Planck constant	h ħ = h/2π	6.626 176 × 10−34 J s 1.054 5887(57) × 10−34 J s	5.4 × 10−6 5.4 × 10−6
Fine structure constant	α = μ0c0e2/2h α−1	0.007 297 3506(60) 137.036 04(11)	8.2 × 10−7 8.2 × 10−7
Gravitational constant	G	6.6720(41) × 10−11 N m2 kg−2	6.15 × 10−4
Rydberg constant	R∞	1.097 373 177(83) × 10−7 m−1	7.5 × 10−8
Elementary charge	e	1.602 1892(46) × 10−19 C	2.9 × 10−6
Avogadro constant	NA	6.022 045(31) × 1023 mol−1	5.1 × 10−6
Atomic mass unit (atomic mass constant)	1 u = (10−3 kg mol−1)/NA mu	1.660 5655(86) × 10−27 kg	5.1 × 10−6
Faraday constant	F = NAe	9.648 456(27) × 104 C mol−1	2.8 × 10−6
Molar gas constant	R	8.314 41(26) J K−1 mol−1	3.1 × 10−5
Boltzmann constant	k = R/NA	1.380 662(44) × 10−23 J K−1	3.2 × 10−5
Molar volume, ideal gas (T0 = 273.15 K, p0 = 1 atm)	Vm = RT0/p0	0.022 413 83(70) m3 mol−1	3.1 × 10−5
Stefan–Bolzmann constant	σ = (π2/60)k4/ħ3c20	5.670 32(71) × 10−8 W m−2 K−4	1.25 × 10−4
First radiation constant	c1 = 2πhc20	3.741 832(20) × 10−16 W m2	5.4 × 10−6
Second radiation constant	c2 = hc0/k	0.014 387 86(45) m K	3.1 × 10−5
Electron rest mass	me	9.109 534(47) × 10−31 kg 5.485 8026(21) × 10−4 u	5.1 × 10−6 3.8 × 10−7
Muon rest mass	mμ	1.883 566(11) × 10−28 kg 0.113 429 20(26) u	5.6 × 10−6 2.3 × 10−6
Proton rest mass	mp	1.672 6485(86) × 10−27 kg 1.007 276 470(11) u	5.1 × 10−6 1.1 × 10−8
Neutron rest mass	mn	1.674 9543(86) × 10−27 kg 1.008 665 012(37) u	5.1 × 10−6 3.7 × 10−8
Ratio, proton mass to electron mass	mp/me	1836.151 52(70)	3.8 × 10−7
Ratio, muon mass to electron mass	mμ/me	206.768 65(47)	2.3 × 10−6
Bohr magneton	μB = eħ/2me	9.274 078(36) × 10−24 J T−1	3.9 × 10−6
Nuclear magneton	μN = eħ/2mp	5.050 824(20) × 10−27 J T−1	3.9 × 10−6
Electron magnetic moment	μe	9.284 832(36) × 10−24 J T−1	3.9 × 10−6
Electron g-factor	½ge = μe/μB	1.001 159 6567(35)	3.5 × 10−9
Muon magnetic moment	μμ	4.490 474(18) × 10−26 J T−1	3.9 × 10−6
Muon g-factor	½gμ	1.001 166 16(31)	3.1 × 10−7
Proton magnetic moment	μp	1.410 6171(55) × 10−26 J T−1	3.9 × 10−6
Proton magnetic moment in Bohr magnetons	μp/μB	1.521 032 209(16) × 10−3	1.1 × 10−8
Proton moment in nuclear magnetons	μp/μN	2.792 8456(11)	3.8 × 10−7
Ratio, electron to proton magnetic moments	μe/μp	658.210 6880(66)	1.0 × 10−8
Ratio, muon moment to proton moment	μμ/μp	3.183 3402(72)	2.3 × 10−6
Proton gyromagnetic ratio	γp	2.675 1987(75) × 108 s−1 T−1	2.8 × 10−6
Diamagnetic shielding factor, spherical H2O sample	1 + σ(H2O)	1.000 025 637(67)	6.7 × 10−8
Proton gyromagnetic ratio (uncorrected)	γp γp/2π	2.675 1301(75) × 108 s−1 T−1 42.576 02(12) MHz T−1	2.8 × 10−6 2.8 × 10−6
Proton moment in nuclear magnetons (uncorrected)	μp/μN	2.792 7740(11)	3.8 × 10−7
Bohr radius	a0 = α/4πR∞	5.291 7706(44) × 10−11 m	8.2 × 10−7
Josephson frequency–voltage ratio (Josephson constant)	e/2h KJ	483.5939(13) THz V−1	2.6 × 10−6
Magnetic flux quantum	Φ0 = h/2e h/e	2.067 8506(54) × 10−15 Wb 4.135 701(11) × 10−15 J Hz−1 C−1	2.6 × 10−6 2.6 × 10−6
Quantum of circulation	h/2me h/me	3.636 9455(60) × 10−4 J Hz−1 kg−1 7.273 891(12) × 10−4 J Hz−1 kg−1	1.6 × 10−6 1.6 × 10−6
Electron Compton wavelength	λC(e) = α2/2R∞ λC(e) = λC(e)/2π = αa0	2.426 3089(40) × 10−12 m 3.861 5905(64) × 10−13 m	1.6 × 10−6 1.6 × 10−6
Proton Compton wavelength	λC(p) = h/mpc0 λC(p) = λC(p)/2π	1.321 4099(22) × 10−15 m 2.103 0892(36) × 10−16 m	1.7 × 10−6 1.7 × 10−6
Neutron Compton wavelength	λC(n) = h/mnc0 λC(n) = λC(n)/2π	1.319 5909(22) × 10−15 m 2.100 1941(35) × 10−16 m	1.7 × 10−6 1.7 × 10−6
Specific electron charge	e/me	1.758 8047(49) × 1011 C kg−1	2.8 × 10−6

Reference

Cohen, E. Richard; Taylor, B. N. The 1973 Least‐Squares Adjustment of the Fundamental Constants. J. Phys. Chem. Ref. Data 1973, 2 (4), 663–734. DOI: 10.1063/1.3253130.