Физическа константа: Разлика между версии

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Ред 149:
!Символ
!Стойност (в [[Международна система единици|SI]])
!Relative standard uncertainty
|-
| colspan="2" |Atomic[[Единица massза constantатомна маса]]
|<math>m_{\text{u}} = 1\,\text{u} </math>
|{{physconst|mu}}
|{{physconst|mu|runc=yes|ref=no}}
|-
| colspan="2" |[[Число на Авогадро]]
|<math>N_{\text{A}}, L </math>
|{{physconst|NA}}
|{{physconst|NA|runc=yes|ref=no}}
|-
| colspan="2" |[[Константа на Болцман]]
|<math>k = k_{\text{B}} = R / N_{\text{A}} </math>
|{{physconst|k}}
|{{physconst|k|runc=yes|ref=no}}
|-
| colspan="2" |[[Константа на Фарадей]]
|<math>F = N_{\text{A}} e </math>
|{{physconst|F}}
|{{physconst|F|runc=yes|ref=no}}
|-
| colspan="2" |първа радиационна константа<br>first radiation constant
|<math>c_1 = 2 \pi h c^2 </math>
|{{physconst|c1}}
|{{physconst|c1|runc=yes|ref=no}}
|-
| colspan="2" |first radiation constant for spectral radiance
|<math>c_{\text{1L}} = c_1/\pi </math>
|{{physconst|c1L}}
|{{physconst|c1L|runc=yes|ref=no}}
|-
| rowspan="2" |LoschmidtКонстанта constantна Лошмит
|<math>T</math> = 273.15&nbsp;K, <math>p</math> = 100&nbsp;kPa
| rowspan="2" |<math>n_0 = N_{\text{A}} / V_{\text{m}} </math>
|2.651 6467(15) × 10<sup>25</sup> m<sup>−3</sup>
|5.7 × 10<sup>−7</sup>
|-
|<math>T</math> = 273.15&nbsp;K, <math>p</math> = 101.325&nbsp;kPa
|2.686 7811(15) × 10<sup>25</sup> m<sup>−3</sup>
|5.7 × 10<sup>−7</sup>
|-
| colspan="2" |[[Универсална газова константа]]
|<math>R </math>
|{{physconst|R}}
|{{physconst|R|runc=yes|ref=no}}
|-
| colspan="2" |molarмоларна Planckконстанта constantна Планк
|<math>N_{\text{A}} h </math>
|{{physconst|NAh}}
|{{physconst|NAh|runc=yes|ref=no}}
|-
| rowspan="2" |[[Моларен обем]] на [[Идеаленидеален газ]]
|<math>T</math> = 273.15&nbsp;K, <math>p</math> = 100&nbsp;kPa
| rowspan="2" |<math>V_{\text{m}} = R T / p </math>
|2.271 0947(13) × 10<sup>−2</sup> m<sup>3</sup>⋅mol<sup>−1</sup>
|5.7 × 10<sup>−7</sup>
|-
|<math>T</math> = 273.15&nbsp;K, <math>p</math> = 101.325&nbsp;kPa
|2.241 3962(13) × 10<sup>−2</sup> m<sup>3</sup>⋅mol<sup>−1</sup>
|5.7 × 10<sup>−7</sup>
|-
| colspan="2" |втора радиационна константа
| rowspan="2" |Sackur–Tetrode constant
|<math>T</math> = 1&nbsp;K, <math>p</math> = 100&nbsp;kPa
| rowspan="2" |<math>S_0 / R = \frac{5}{2}</math> <br /><br /><math> + \ln\left[ (2\pi m_{\text{u}} k T / h^2)^{3/2} k T / p \right]</math>
|−1.151 7084(14)
|1.2 × 10<sup>−6</sup>
|-
|<math>T</math> = 1&nbsp;K, <math>p</math> = 101.325&nbsp;kPa
|−1.164 8714(14)
|1.2 × 10<sup>−6</sup>
|-
| colspan="2" |second radiation constant
|<math>c_2 = h c / k </math>
|{{physconst|c2}}
|{{physconst|c2|runc=yes|ref=no}}
|-
| colspan="2" |[[Константа на Стефан – Болцман]]
|<math>\sigma = \pi^2 k^4 / 60 \hbar^3 c^2 </math>
|{{physconst|sigma}}
|{{physconst|sigma|runc=yes|ref=no}}
|-
| colspan="2" |Wien wavelength displacement law constant
|<math>b</math>
|{{physconst|bwien}}
|{{physconst|bwien|runc=yes|ref=no}}
|-
| colspan="2" |Wien frequency displacement law constant
|<math>b'</math>
|{{physconst|bwien'}}
|{{physconst|bwien'|runc=yes|ref=no}}
|-
| colspan="2" |Wien-Bonal entropy displacement law constant<ref>{{Cite journal|last1=Delgado-Bonal|first1=Alfonso|title=Entropy of radiation: the unseen side of light|journal=Scientific Reports|date=10 May 2017|volume=7|issue=1642|doi=10.1038/s41598-017-01622-6}}</ref>
|<math>b_\text{entropy}</math>
|3.002 9152(05) × 10<sup>−3</sup> m⋅K
|5.7 × 10<sup>−7</sup>
|-
|}