Physical constant
In science, the physical constant is the name given to the value of a physical magnitude that, given a system of units, remains invariable in physical processes over time. In contrast, a mathematical constant represents an unchanging value that is not directly involved in any physical process.
There are many physical constants; some of the best known are Planck's reduced constant ( {displaystyle hbar }), the gravitation constant (G{displaystyle G}), the speed of light (c{displaystyle c}), allowivity in the void (ε ε 0{displaystyle epsilon}), magnetic permeability in the vacuum (μ μ 0{displaystyle mu _{0}}) and the elementary load (e{displaystyle e}). All these, being so fundamental, are called universal constants.
On the other hand, since 1937 Paul Dirac and other scientists have speculated that the value of physical constants might decrease in proportion to the age of the Universe. To date, no experiment has indicated that this is the case, although it has been possible to calculate the maximum levels of this hypothetical variation of the constants. The maximum levels of annual variation are, in any case, very small, being 10-5 for the fine structure and 10-11 for the gravitation constant. The issue is still a matter of controversy today.
Some considerations
Dimensional and dimensionless constants
Physical constants can have dimensions such as, for example, the speed of light in the vacuum (which in the SI is expressed in meters per second), while others, such as the constant of fine structure (α α {displaystyle alpha }) that characterizes the interaction between electrons and photons, is dimensional.
Unless natural units are used, the value of constants that have dimensions will depend on the unit system used. By contrast, dimensionless constants are independent of the system of units used and are known as fundamental physical constants. The fine structure constant is probably the best known of these dimensionless constants. The ratios of the masses (or other properties) of the particles are also fundamental physical constants.
Physical constants and life in the Universe
In many of these constants a precise adjustment occurs that makes the existence of the human being in the cosmos compatible. If the value of certain of those constants were only slightly different from what they possess, the Universe would have to be radically different, making it impossible for life as we know it to emerge. The fact that the Universe is properly calibrated and adjusted to accommodate intelligent life has intrigued many and has also been the subject of scientific and philosophical debate. Perhaps one of the best answers that explains the adjustment of the constants is the one given by the anthropic principle. This affirms that since the human being is here, the Universe must be a universe capable of housing it and, therefore, it is not possible to wonder about the possibility that these values were different since, if so, there would be no one who could ask him.
Tables of physical constants
- NOTE: Although many properties of materials and particles are constant, they are not shown in tables as they are specific to the respective materials or particles.
Table of universal constants
Amount | Symbol | Value | Relative error |
---|---|---|---|
Vacuum characteristic impedance | Z0=μ μ 0c{displaystyle Z_{0}=mu _{0}c,} | 376,730 313 461... Ω | defined |
Electrical vacuum permit | ε ε 0{displaystyle epsilon _{0},} | 8,854 187 817... × 10-12 F·m-1 | defined |
Magnetic Permeability of Vacuum | μ μ 0{displaystyle mu _{0},} | 4π × 10-7 N·A-2 = 1,2566 370 614... × 10-6 N·A-2 | defined |
Constant universal gravitation | G{displaystyle G,} | 6,671 91(99) × 10-11 N·m2/kg2 | 1.5 × 10-6 |
Constant of Planck | h{displaystyle h,} | 6,626 070 15 × 10- 34 J·s | defined |
Reduced Constant of Planck | =h2π π {displaystyle hbar ={frac {h}{2pi }}}} | 1,054 571 817 646 16 × 10- 34 J·s | Exactly |
Speed of light in the vacuum | c=1μ μ 0ε ε 0{displaystyle c={frac {1}{sqrt {mu _{0}epsilon _{0}}}}{,} | 299 792 458 m·s-1 | defined |
Table of electromagnetic constants
Amount | Symbol | Value1 (units SI) | Relative error |
---|---|---|---|
Bohr Magneton | μ μ B=e /2me{displaystyle mu _{B}=ehbar /2m_{e}} | 9,27400949(80) × 10-24 J·T-1 | 8.6 × 10-8 |
Nuclear Magneton | μ μ N=e /2mp{displaystyle mu _{N}=ehbar /2m_{p}}} | 5,050 783 43(43) × 10-27 J·T-1 | 8.6 × 10-8 |
Quantum resistance | R0=h/2e2{displaystyle R_{0}=h/2e^{2},} | 12 906,403 729 652 3 Ω | Exactly |
Constant von Klitzing | RK=h/e2{displaystyle R_{K}=h/e^{2},} | 25 812.807 459 304 5 Ω | Exactly |
Table of atomic and nuclear constants
Amount | Symbol | Value1 (units SI) | Relative error | |
Radio de Bohr | a0=α α /4π π R∞ ∞ {displaystyle a_{0}=alpha /4pi R_{infty },} | 0.529 177 2108(18) × 10-10 m | 3.3 × 10-9 | |
Fermi coupling Constant | GF/( c)3{displaystyle G_{F}/(hbar c)^{3} | 1,166 39(1) × 10-5 GeV-2 | 8.6 × 10-6 | |
Consisting of fine structure | α α =μ μ 0e2c/(2h)=e2/(4π π ε ε 0 c){displaystyle alpha =mu _{0}e^{2}c/(2h)=e^{2}/(4pi epsilon _{0}hbar c),} | 7,297 352 568(24) × 10-3 | 3.3 × 10-9 | |
Hartree Energy | Eh=2R∞ ∞ hc{displaystyle E_{h}=2R_{infty }hc,} | 4,359 744 17(75) × 10-18 J | 1.7 × 10-7 | |
Quantum of circulation | h/2me{displaystyle h/2m_{e},} | 3,636 947 550(24) × 10-4 m2 s-1 | 6.7 × 10-9 | |
Rydberg Constant | R∞ ∞ =α α 2mec/2h{displaystyle R_{infty }=alpha ^{2}m_{ec/2h,} | 10 973 731.568 525(73) m-1 | 6,6 × 10-12 | |
Effective Thomson Section | (8π π /3)re2{displaystyle (8pi /3)r_{e}^{2}} | 0.665 245 873(13) × 10- 28 m2 | 2.0 × 10-8 | |
Weinberg Angle | without2 θ θ W=1− − (mW/mZ)2{displaystyle sin ^{2}theta _{W}=1-(m_{W}/m_{Z})^{2},} | 0.222 15(76) | 3.4 × 10-3 |
Table of physical-chemical constants
Amount | Symbol | Value1 (units SI) | Relative error | |
Constant atomic mass | mu=1u{displaystyle m_{u}=1 u,} | 1,660 538 86(28) × 10-27 kg | 1.7 × 10-7 | |
Number of Avogadro | NA,L{displaystyle N_{A},L,} | 6,022 140 76 × 1023 | defined | |
Boltzmann Constant | k=R/NA{displaystyle k=R/N_{A},} | 1,380 649 × 10-23 J·K-1 | defined | |
Constant Faraday | F=NAe{displaystyle F=N_{A}e,} | 96 485,332 123 310 018 4 C·mol-1 | Exactly | |
First radiation constant | c1=2π π hc2{displaystyle c_{1}=2pi hc^{2},} | 3,741 771 852 191 76 × 10-16 W·m2 | Exactly | |
for spectral radiance | c1L{displaystyle c_{1L},} | 1,191 042 82(20) × 10-16 W · m2 sr-1 | 1.7 × 10-7 | |
Number of Loschmidt | a T{displaystyle T}=273.15 K and p{displaystyle p}=101.325 kPa | n0=NA/Vm{displaystyle n_{0}=N_{A}/V_{m},} | 2,686 7773(47) × 1025 m-3 | 1.8 × 10-6 |
Universal consistency of ideal gases | R{displaystyle R,} | 8.314 462 618 153 24 J·K-1·mol-1 | Exactly | |
Constant molar of Planck | NAh{displaystyle N_{A}h,} | 3,990 312 712 893 431 4 × 10-10 J · s · mol-1 | Exactly | |
Molar volume of an ideal gas | a T{displaystyle T}=273.15 K and p{displaystyle p}= 100 kPa | Vm=RT/p{displaystyle V_{m}=RT/p,} | 22,710 981(40) × 10-3 m3 · mol-1 | 1.7 × 10-6 |
a 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 | ||
Sackur-Tetrode Constant | a T{displaystyle T}=1 K and p{displaystyle p}= 100 kPa | S0/R=52{displaystyle S_{0}/R={frac {5}{2}}}}} +ln [chuckles](2π π mukT/h2)3/2kT/p]{displaystyle +ln left[(2pi m_{u}kT/h^{2}}{3/2}kT/pright]}} | -1,151 7047(44) | 3.8 x 10-6 |
a T{displaystyle T}=1 K and p{displaystyle p}=101.325 kPa | -1.164 8677(44) | 3.8 x 10-6 | ||
Second radiation constant | c2=hc/k{displaystyle c_{2}=hc/k,} | 1,438 776 877 503 93 × 10-2 m·K | Exactly | |
Constant Stefan-Boltzmann | σ σ =(π π 2/60)k4/ 3c2{displaystyle sigma =(pi ^{2}/60)k^{4}/hbar ^{3}c^{2}} | 5.670 374 419 184 43 × 10-8 W·m-2·K-4 | Exactly | |
Constant of the Displacement Act of Wien | benergia=(hc/k)/{displaystyle b_{energia}=(hc/k)/,} 4,965 114 231... | 2,897 7685(51) × 10-3 m · K | 1.7 × 10-6 | |
Conventional value of Josephson's constant2 | KJ− − 90{displaystyle K_{J-90},} | 483 597,9 × 109 Hz · V-1 | defined |
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