Lihat sumber Templat:Table of physico-chemical constants

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!colspan=2|{{tnavbar-header|Quantity|Table of physico-chemical constants}}
!Simbol
!Nilai<ref name="concise">The values are given in the so-called ''concise form''; the number in parentheses after the [[Significand|mantissa]] is the ''[[ketidakpastian standar]]'', which is the value multiplied by the ''[[ketidakpastian standar relatif]]'', and indicates the amount by which the [[least significant digit]]s of the value are uncertain. For example, 75 is the standard uncertainty in "8.314 4621(75)", and means that the value is between 8.314 4546 and 8.314 4696.</ref><ref name="2010 CODATA">P.J. Mohr, B.N. Taylor, and D.B. Newell (2011), "The 2010 CODATA Recommended Values of the Fundamental Physical Constants" (Web Version 6.0). This database was developed by J. Baker, M. Douma, and S. Kotochigova. Available: http://physics.nist.gov/constants [Thursday, 02-Jun-2011 21:00:12 EDT]. National Institute of Standards and Technology, Gaithersburg, MD 20899.</ref> (satuan [[SI]])
!Ketidakpastian standar relatif
|-
|colspan=2|[[konstanta massa atom]]
|<math>m_{\mathrm{u}} = 1\,\mathrm{u} \,</math>
|1.660 538 921(73) × 10<sup>−27</sup> kg
|4.4 × 10<sup>−8</sup>
|-
|colspan=2|[[bilangan Avogadro]]
|<math>N_{\mathrm{A}}, L \,</math>
|6.022 141 29(27) × 10<sup>23</sup> mol<sup>−1</sup>
|4.4 × 10<sup>−8</sup>
|-
|colspan=2|[[konstanta Boltzmann]]
|<math>k = k_{\mathrm{B}} = R / N_{\mathrm{A}} \,</math>
|1.380 6488(13) × 10<sup>−23</sup> J·K<sup>−1</sup>
|9.1 × 10<sup>−7</sup>
|-
|colspan=2|[[konstanta Faraday]]
|<math>F = N_{\mathrm{A}} e \,</math>
|96 485.3365(21)C·mol<sup>−1</sup>
|2.2 × 10<sup>−8</sup>
|-
|rowspan=2|konstanta radiasi pertama
| 
|<math>c_1 = 2 \pi h c^2 \,</math>
|3.741 771 53(17) × 10<sup>−16</sup> W·m<sup>2</sup>
|4.4 × 10<sup>−8</sup>
|-
|untuk radiansi spektral
|<math>c_{\mathrm{1L}} = c_1/\pi \,</math>
|1.191 042 869(53) × 10<sup>−16</sup> W·m<sup>2</sup>·sr<sup>−1</sup>
|4.4 × 10<sup>−8</sup>
|-
|[[konstanta Loschmidt]]
|at <math>T</math>=273.15 K and <math>p</math>=101.325 kPa
|<math>n_0 = N_{\mathrm{A}} / V_{\mathrm{m}} \,</math>
|2.686 7805(24) × 10<sup>25</sup> m<sup>−3</sup>
|9.1 × 10<sup>−7</sup>
|-
|colspan=2|[[konstanta gas]]
|<math>R \,</math>
|8.314 4621(75) J·K<sup>−1</sup>·mol<sup>−1</sup>
|9.1 × 10<sup>−7</sup>
|-
|colspan=2|konstanta molar Planck 
|<math>N_{\mathrm{A}} h \,</math>
|3.990 312 7176(28) × 10<sup>−10</sup> J·s·mol<sup>−1</sup>
|7.0 × 10<sup>−10</sup>
|-
|rowspan=2|[[volume molar]] [[gas ideal]]
|pada <math>T</math>=273.15 K and <math>p</math>=100 kPa
|rowspan=2|<math>V_{\mathrm{m}} = R T / p \,</math>
|2.271 0953(21) × 10<sup>−2</sup> m<sup>3</sup>·mol<sup>−1</sup>
|9.1 × 10<sup>−7</sup>
|-
|pada <math>T</math>=273.15 K and <math>p</math>=101.325 kPa
|2.241 3968(20) × 10<sup>−2</sup> m<sup>3</sup>·mol<sup>−1</sup>
|9.1 × 10<sup>−7</sup>
|-
|rowspan=2 style="text-align:center;"|[[konstanta Sackur-Tetrode]]
|pada <math>T</math>=1 K and <math>p</math>=100 kPa
|rowspan=2|<math>S_0 / R = \frac{5}{2}</math> <br><math> + \ln\left[ (2\pi m_{\mathrm{u}} k T / h^2)^{3/2} k T / p \right]</math>
|−1.151 7078(23)
|2.0 × 10<sup>−6</sup>
|-
|pada <math>T</math>=1 K and <math>p</math>=101.325 kPa
|−1.164 8708(23)
|1.9 × 10<sup>−6</sup>
|-
|colspan=2|konstanta radiasi kedua
|<math>c_2 = h c / k \,</math>
|1.438 7770(13) × 10<sup>−2</sup> m·K
|9.1 × 10<sup>−7</sup>
|-
|colspan=2|[[konstanta Stefan–Boltzmann]]
|<math>\sigma = \pi^2 k^4 / 60 \hbar^3 c^2 </math>
|5.670 373(21) × 10<sup>−8</sup> W·m<sup>−2</sup>·K<sup>−4</sup>
|3.6 × 10<sup>−6</sup>
|-
|colspan=2|[[Hukum perpindahan Wien|konstanta hukum perpindahan Wien]]
|<math>b = h c k^{-1} / \,</math> 4.965 114 231...
|2.897 7721(26) × 10<sup>−3</sup> m·K
|9.1 × 10<sup>−7</sup>
|-
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