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Vacuum permittivity

From Wikipedia, the free encyclopedia
Absolute dielectric permittivity of free space

This article is about the electric constant. For the analogous magnetic constant, seeVacuum permeability. For the ordinal number ε0, seeEpsilon numbers (mathematics).
Value ofε0Unit
8.8541878188(14)×10−12Fm−1
C2kg−1m−3s2
55.26349406e2eV−1μm−1

Vacuum permittivity, commonly denotedε0 (pronounced "epsilon nought" or "epsilon zero"), is the value of theabsolute dielectric permittivity ofclassical vacuum. It may also be referred to as thepermittivity of free space, theelectric constant, or the distributed capacitance of the vacuum. It is an ideal (baseline)physical constant. ItsCODATA value is:

ε0 = 8.8541878188(14)×10−12 F⋅m−1.[1]

It is a measure of how dense of anelectric field is "permitted" to form in response to electric charges and relates the units forelectric charge to mechanical quantities such as length and force.[2] For example, the force between two separated electric charges with spherical symmetry (in thevacuum of classical electromagnetism) is given byCoulomb's law:FC=14πε0q1q2r2{\displaystyle F_{\text{C}}={\frac {1}{4\pi \varepsilon _{0}}}{\frac {q_{1}q_{2}}{r^{2}}}}Here,q1 andq2 are the charges,r is the distance between their centres, and the value of the constant fraction 1/(4πε0) is approximately9×109 N⋅m2⋅C−2. Likewise,ε0 appears inMaxwell's equations, which describe the properties ofelectric andmagnetic fields andelectromagnetic radiation, and relate them to their sources. Inelectrical engineering,ε0 itself is used as a unit to quantify the permittivity of variousdielectric materials.

Value

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The value ofε0 obeys the formula[3]ε0=1μ0c2{\displaystyle \varepsilon _{0}={\frac {1}{\mu _{0}c^{2}}}}wherec is the defined value for thespeed of light inclassical vacuum inSI units,[4]: 127  andμ0 is the parameter that international standards organizations refer to as themagnetic constant (also calledvacuum permeability or the permeability of free space). Sinceμ0 has an approximate value of 4π × 10−7 H/m (by the former definition of theampere),[4][5] andc has thedefined value299792458 m/s, it follows thatε0 can be expressed numerically as[6]ε01(4π×107N/A2)(299792458m/s)28.8541878176×1012F/m.{\displaystyle \varepsilon _{0}\approx {\frac {1}{\left(4\pi \times {10}^{-7}\,\mathrm {N/A^{2}} \right){\left(299\,792\,458\,\mathrm {m/s} \right)}^{2}}}\approx {8.854\,187\,8176}\times {10}^{-12}\,\mathrm {F/m} .}The relative deviation of the recommended measured value (1.3×10−10 or 0.13 parts per billion) from the former defined value is within its uncertainty (1.6×10−10, in relative terms, or 0.16 parts per billion).

The historical origins of the electric constantε0, and its value, are explained in more detail below.

Revision of the SI

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Main article:2019 revision of the SI

Theelementary charge was redefined exactly in terms of the coulomb as from 20 May 2019,[4] with the effect that the vacuum electric permittivity and themagnetic vacuum permeability no longer have exactly determined values in SI units. The value of the electron charge became a numerically defined quantity, makingε0 andμ0 measured quantities, neither of them exact, but related by the equationε0μ0c2 = 1. These values are determined by the experimentally determinedfine-structure constantα:ε0=1μ0c2=e22αhc ,{\displaystyle \varepsilon _{0}={\frac {1}{\mu _{0}c^{2}}}={\frac {e^{2}}{2\alpha hc}}\ ,}withe being theelementary charge,h being thePlanck constant, andc being thespeed of light invacuum, each with exactly defined values. The relative uncertainty in the values of each ofε0 andμ0 are therefore the same as that for thefine-structure constant, namely1.6×10−10.[7]

Terminology

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Historically, the parameterε0 has been known by many different names. The terms "vacuum permittivity" or its variants, such as "permittivity in/of vacuum",[8][9] "permittivity of empty space",[10] or "permittivity offree space"[11] are widespread. Standards organizations also use "electric constant" as a term for this quantity.[12][13]

Another historical synonym was "dielectric constant of vacuum", as "dielectric constant" was sometimes used in the past for the absolute permittivity.[14][15] However, in modern usage "dielectric constant" typically refers exclusively to arelative permittivityε/ε0 and even this usage is considered "obsolete" by some standards bodies in favor ofrelative static permittivity.[13][16] Hence, the term "dielectric constant of vacuum" for the electric constantε0 is considered obsolete by most modern authors, although occasional examples of continuing usage can be found.

As for notation, the constant can be denoted by eitherε0 orϵ0, using either of the commonglyphs for the letterepsilon.

Historical origin of the parameterε0

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As indicated above, the parameterε0 is a measurement-system constant. Its presence in the equations now used to define electromagnetic quantities is the result of the so-called "rationalization" process described below. But the method of allocating a value to it is a consequence of the result that Maxwell's equations predict that, in free space, electromagnetic waves move with the speed of light. Understanding whyε0 has the value it does requires a brief understanding of the history.

Rationalization of units

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The experiments ofCoulomb and others showed that the forceF between two, equal, point-like "amounts" of electricity that are situated a distancer apart in free space, should be given by a formula that has the formF=keQ2r2,{\displaystyle F=k_{\text{e}}{\frac {Q^{2}}{r^{2}}},}whereQ is a quantity that represents the amount of electricity present at each of the two points, andke depends on the units. If one is starting with no constraints, then the value ofke may be chosen arbitrarily.[17] For each different choice ofke there is a different "interpretation" ofQ: to avoid confusion, each different "interpretation" has to be allocated a distinctive name and symbol.

In one of the systems of equations and units agreed in the late 19th century, called the "centimetre–gram–second electrostatic system of units" (the cgs esu system), the constantke was taken equal to 1, and a quantity now called "Gaussian electric charge"qs was defined by the resulting equationF=qs2r2.{\displaystyle F={\frac {{q_{\text{s}}}^{2}}{r^{2}}}.}

The unit of Gaussian charge, thestatcoulomb, is such that two units, at a distance of 1 centimetre apart, repel each other with a force equal to the cgs unit of force, thedyne. Thus, the unit of Gaussian charge can also be written 1 dyne1/2⋅cm. "Gaussian electric charge" is not the same mathematical quantity as modern (MKS and subsequently theSI) electric charge and is not measured in coulombs.

The idea subsequently developed that it would be better, in situations of spherical geometry, to include a factor 4π in equations like Coulomb's law, and write it in the form:F=keqs24πr2.{\displaystyle F=k'_{\text{e}}{\frac {{q'_{\text{s}}}^{2}}{4\pi r^{2}}}.}

This idea is called "rationalization". The quantitiesqs′ andke′ are not the same as those in the older convention. Puttingke′ = 1 generates a unit of electricity of different size, but it still has the same dimensions as the cgs esu system.

The next step was to treat the quantity representing "amount of electricity" as a fundamental quantity in its own right, denoted by the symbolq, and to write Coulomb's law in its modern form: F=14πε0q2r2.{\displaystyle \ F={\frac {1}{4\pi \varepsilon _{0}}}{\frac {q^{2}}{r^{2}}}.}

The system of equations thus generated is known as the rationalized metre–kilogram–second (RMKS) equation system, or "metre–kilogram–second–ampere (MKSA)" equation system. The new quantityq is given the name "RMKS electric charge", or (nowadays) just "electric charge".[citation needed] The quantityqs used in the old cgs esu system is related to the new quantityq by: qs=q4πε0.{\displaystyle \ q_{\text{s}}={\frac {q}{\sqrt {4\pi \varepsilon _{0}}}}.}

In the2019 revision of the SI, the elementary charge is fixed at1.602176634×10−19 C and the value of the vacuum permittivity must be determined experimentally.[18]: 132 

Determination of a value forε0

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One now adds the requirement that one wants force to be measured in newtons, distance in metres, and charge to be measured in the engineers' practical unit, the coulomb, which is defined as the charge accumulated when a current of 1 ampere flows for one second. This shows that the parameterε0 should be allocated the unit C2⋅N−1⋅m−2 (or an equivalent unit – in practice, farad per metre).

In order to establish the numerical value ofε0, one makes use of the fact that if one uses the rationalized forms of Coulomb's law andAmpère's force law (and other ideas) to developMaxwell's equations, then the relationship stated above is found to exist betweenε0,μ0 andc0. In principle, one has a choice of deciding whether to make the coulomb or the ampere the fundamental unit of electricity and magnetism. The decision was taken internationally to use the ampere. This means that the value ofε0 is determined by the values ofc0 andμ0, as stated above. For a brief explanation of how the value ofμ0 is decided, seeVacuum permeability.

Permittivity of real media

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By convention, the electric constantε0 appears in the relationship that defines theelectric displacement fieldD in terms of theelectric fieldE and classical electricalpolarization densityP of the medium. In general, this relationship has the form:D=ε0E+P.{\displaystyle \mathbf {D} =\varepsilon _{0}\mathbf {E} +\mathbf {P} .}

For a linear dielectric,P is assumed to be proportional toE, but a delayed response is permitted and a spatially non-local response, so one has:[19]D(r, t)=tdtd3rε(r, t;r, t)E(r, t).{\displaystyle \mathbf {D} (\mathbf {r} ,\ t)=\int _{-\infty }^{t}dt'\int d^{3}\mathbf {r} '\,\varepsilon {\left(\mathbf {r} ,\ t;\mathbf {r} ',\ t'\right)}\,\mathbf {E} {\left(\mathbf {r} ',\ t'\right)}.}

In the event that nonlocality and delay of response are not important, the result is:D=εE=εrε0E{\displaystyle \mathbf {D} =\varepsilon \mathbf {E} =\varepsilon _{\text{r}}\varepsilon _{0}\mathbf {E} }whereε is thepermittivity andεr therelative static permittivity. In thevacuum of classical electromagnetism, the polarizationP =0, soεr = 1 andε =ε0.

See also

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Notes

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  1. ^"2022 CODATA Value: vacuum electric permittivity".The NIST Reference on Constants, Units, and Uncertainty.NIST. May 2024. Retrieved18 May 2024.
  2. ^"electric constant".Electropedia: International Electrotechnical Vocabulary (IEC 60050). Geneva: International Electrotechnical Commission. Retrieved26 March 2015..
  3. ^The approximate numerical value is found at:"–: Electric constant,ε0".NIST reference on constants, units, and uncertainty: Fundamental physical constants. NIST. Retrieved22 January 2012. This formula determining the exact value ofε0 is found in Table 1, p. 637 ofPJ Mohr; BN Taylor; DB Newell (April–June 2008)."Table 1: Some exact quantities relevant to the 2006 adjustment inCODATA recommended values of the fundamental physical constants: 2006"(PDF).Rev Mod Phys.80 (2):633–729.arXiv:0801.0028.Bibcode:2008RvMP...80..633M.doi:10.1103/RevModPhys.80.633.
  4. ^abcThe International System of Units(PDF), V3.01 (9th ed.), International Bureau of Weights and Measures, August 2024,ISBN 978-92-822-2272-0
  5. ^See the last sentence of theNIST definition of ampere.
  6. ^A summary of the definitions ofc,μ0 andε0 is provided in the 2006 CODATA Report:CODATA report, pp. 6–7
  7. ^"2022 CODATA Value: fine-structure constant".The NIST Reference on Constants, Units, and Uncertainty.NIST. May 2024. Retrieved18 May 2024.
  8. ^Sze, S. M. & Ng, K. K. (2007)."Appendix E".Physics of semiconductor devices (Third ed.). New York: Wiley-Interscience. p. 788.ISBN 978-0-471-14323-9.
  9. ^Muller, R. S.; T. I., Kamins & Chan, M. (2003).Device electronics for integrated circuits (3rd ed.). New York: Wiley. Inside front cover.ISBN 978-0-471-59398-0.
  10. ^Sears, F. W.; Zemansky, M. W. & Young, H. D. (1985).College physics. Reading, Massachusetts: Addison-Wesley. p. 40.ISBN 978-0-201-07836-7.
  11. ^B. E. A. Saleh and M. C. Teich,Fundamentals of Photonics (Wiley, 1991)
  12. ^International Bureau of Weights and Measures (2006),The International System of Units (SI)(PDF) (8th ed.), p. 104,ISBN 92-822-2213-6,archived(PDF) from the original on 4 June 2021, retrieved16 December 2021
  13. ^abBraslavsky, S. E. (2007)."Glossary of terms used in photochemistry (IUPAC recommendations 2006)"(PDF).Pure and Applied Chemistry.79 (3):293–465, see p. 348.doi:10.1351/pac200779030293.S2CID 96601716.
  14. ^"Naturkonstanten".Freie Universität Berlin. Archived fromthe original on 1 July 2016. Retrieved12 February 2008.
  15. ^King, Ronold W. P. (1963).Fundamental Electromagnetic Theory. New York: Dover. p. 139.
  16. ^IEEE Standards Board (1997).IEEE Standard Definitions of Terms for Radio Wave Propagation. p. 6.doi:10.1109/IEEESTD.1998.87897.ISBN 978-0-7381-0580-2.
  17. ^For an introduction to the subject of choices for independent units, seeJackson, John David (1999)."Appendix on units and dimensions".Classical electrodynamics (Third ed.). New York: Wiley. pp. 775et seq.ISBN 978-0-471-30932-1.
  18. ^"SI Brochure" (9th ed.). BIPM. 2019. Retrieved20 May 2019.
  19. ^Jenö Sólyom (2008)."Equation 16.1.50".Fundamentals of the physics of solids: Electronic properties. Springer. p. 17.ISBN 978-3-540-85315-2.
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