Pemalar fizik

Dalam fizik, pemalar fizik merupakan kuantiti fizikal yang dipercayai mempunyai nilai sejagat yang tetap (malar). Ia dikira daripada kuantiti fizikal yang lain.

Contohnya, cas asas, e mempunyai nilai 1.602 176 487 × 10-19 C.

Jadual pemalar universal

Kuantiti Simbol Nilai Ketakpastian relatif piawai
impedans vakum berciri Z 0 = μ 0 c {\displaystyle Z_{0}=\mu _{0}c\,} 376.730 313 461... Ω ditakrif
pemalar elektrik (ketelusan vakum) ϵ 0 = 1 / ( μ 0 c 2 ) {\displaystyle \epsilon _{0}=1/(\mu _{0}c^{2})\,} 8.854 187 817... × 10-12F·m-1 ditakrif
pemalar magnet (ketelusan vakum) μ 0 {\displaystyle \mu _{0}\,} 4π × 10-7 N·A-2 = 1.256 637 061... × 10-6 N·A-2 ditakrif
pemalar graviti G {\displaystyle G\,} 6.67428(67) × 10-11m3·kg-1·s-2 1.0 × 10-4
pemalar Planck h {\displaystyle h\,} 6.626 068 96(33) × 10-34 J·s 5.0 × 10-8
pemalar Dirac (pemalar Planck terturun) = h / ( 2 π ) {\displaystyle \hbar =h/(2\pi )} 1.054 571 628(53) × 10-34 J·s 5.0 × 10-8
kelajuan cahaya di vakum c {\displaystyle c\,} 299 792 458 m·s-1 ditakrif

Pemalar fizik-kimia

Kuantiti Simbol Nilai1 (SI) Ketakpastian relatif piawai
unit jisim atom m u = 1   u {\displaystyle m_{u}=1\ u\,} 1.660 538 86(28) × 10-27 kg 1.7 × 10-7
pemalar Avogadro N A , L {\displaystyle N_{A},L\,} 6.022 1415(10) × 1023 1.7 × 10-7
pemalar Boltzmann k = R / N A {\displaystyle k=R/N_{A}\,} 1.380 6505(24) × 10-23 J·K-1 1.8 × 10-6
pemalar Faraday F = N A e {\displaystyle F=N_{A}e\,} 96 485.3383(83)C·mol-1 8.6 × 10-8
pemalar sinaran pertama c 1 = 2 π h c 2 {\displaystyle c_{1}=2\pi hc^{2}\,} 3.741 771 38(64) × 10-16 W·m2 1.7 × 10-7
bagi kesinaran spektrum c 1 L {\displaystyle c_{1L}\,} 1.191 042 82(20) × 10-16 W · m2 sr-1 1.7 × 10-7
pemalar Loschmidt at T {\displaystyle T} =273.15 K and p {\displaystyle p} =101.325 kPa n 0 = N A / V m {\displaystyle n_{0}=N_{A}/V_{m}\,} 2.686 7773(47) × 1025 m-3 1.8 × 10-6
pemalar gas R {\displaystyle R\,} 8.314 472(15) J·K-1·mol-1 1.7 × 10-6
pemalar Planck molar N A h {\displaystyle N_{A}h\,} 3.990 312 716(27) × 10-10 J · s · mol-1 6.7 × 10-9
isi padu molar gas ideal at T {\displaystyle T} =273.15 K and p {\displaystyle p} =100 kPa V m = R T / p {\displaystyle V_{m}=RT/p\,} 22.710 981(40) × 10-3 m3 ·mol-1 1.7 × 10-6
pada T {\displaystyle T} =273.15 K and p {\displaystyle p} =101.325 kPa 22.413 996(39) × 10-3 m3 ·mol-1 1.7 × 10-6
pemalar Sackur-Tetrode at T {\displaystyle T} =1 K and p {\displaystyle p} =100 kPa S 0 / R = 5 2 {\displaystyle S_{0}/R={\frac {5}{2}}}
+ ln [ ( 2 π m u k T / h 2 ) 3 / 2 k T / p ] {\displaystyle +\ln \left[(2\pi m_{u}kT/h^{2})^{3/2}kT/p\right]}
-1.151 7047(44) 3.8 × 10-6
pada T {\displaystyle T} =1 K and p {\displaystyle p} =101.325 kPa -1.164 8677(44) 3.8 × 10-6
pemalar sinaran kedua c 2 = h c / k {\displaystyle c_{2}=hc/k\,} 1.438 7752(25) × 10-2 m·K 1.7 × 10-6
pemalar Stefan-Boltzmann σ = ( π 2 / 60 ) k 4 / 3 c 2 {\displaystyle \sigma =(\pi ^{2}/60)k^{4}/\hbar ^{3}c^{2}} 5.670 400(40) × 10-8 W·m-2·K-4 7.0 × 10-6
pemalar hukum sesaran Wien b = ( h c / k ) / {\displaystyle b=(hc/k)/\,} 4.965 114 231... 2.897 7685(51) × 10-3 m · K 1.7 × 10-6

Nilai diakui

Kuantiti Simbol Nilai (SI) Ketakpastian relatif piawai
pemalar Josephson2 K J 90 {\displaystyle K_{J-90}\,} 483 597.9 × 109 Hz · V-1 ditakrif
pemalar von Klitzing3 R K 90 {\displaystyle R_{K-90}\,} 25 812.807 Ω ditakrif
jisim molar pemalar M u = M ( 12 C ) / 12 {\displaystyle M_{u}=M(\,^{12}{\mbox{C}})/12} 1 × 10-3 kg · mol-1 ditakrif
bagi karbon-12 M ( 12 C ) = N A m ( 12 C ) {\displaystyle M(\,^{12}{\mbox{C}})=N_{A}m(\,^{12}{\mbox{C}})} 12 × 10-3 kg · mol−1 ditakrif
pecutan graviti g n {\displaystyle g_{n}\,\!} 9.806 65 m·s-2 ditakrif
atmosfera piawai atm {\displaystyle {\mbox{atm}}\,} 101 325 Pa ditakrif