Volt: Difference between revisions
HeyElliott (talk | contribs) |
Removing {{AFI}}, article for improvement period has concluded |
||
(47 intermediate revisions by 32 users not shown) | |||
Line 1: | Line 1: | ||
{{Short description|SI derived unit of voltage}} |
{{Short description|SI derived unit of voltage}} |
||
{{Update|date=November 2024}} |
|||
{{Other uses}} |
{{Other uses}} |
||
{{Use dmy dates|date=December 2024}} |
|||
{{Infobox Unit |
{{Infobox Unit |
||
| name = volt |
| name = volt |
||
Line 14: | Line 16: | ||
}} |
}} |
||
The '''volt''' (symbol: '''V''') is the unit of [[electric potential]], [[electric potential difference]] ([[voltage]]), and [[electromotive force]] in the [[International System of Units|International System of Units (SI)]].<ref>{{cite web| |
The '''volt''' (symbol: '''V''') is the unit of [[electric potential]], [[Voltage#Galvani potential vs. electrochemical potential|electric potential difference]] ([[voltage]]), and [[electromotive force]] in the [[International System of Units|International System of Units (SI)]].<ref>{{cite web |url=http://www.bipm.org/en/si/si_brochure/chapter2/2-2/table3.html |title=SI Brochure, Table 3 (Section 2.2.2) |access-date=29 July 2007 |year=2006 |publisher=BIPM |archive-url=https://web.archive.org/web/20070618123613/http://www.bipm.org/en/si/si_brochure/chapter2/2-2/table3.html |archive-date=18 June 2007}}</ref> |
||
== Definition == |
== Definition == |
||
One volt is defined as the |
One volt is defined as the electric potential between two points of a [[electrical conductor|conducting wire]] when an [[electric current]] of one [[ampere]] dissipates one [[watt]] of [[power (physics)|power]] between those points.<ref>[https://www.bipm.org/documents/20126/41483022/si-brochure-9-App1-EN.pdf BIPM SI Brochure: Appendix 1] {{Webarchive|url=https://web.archive.org/web/20220227145519/https://www.bipm.org/documents/20126/41483022/si-brochure-9-App1-EN.pdf |date=27 February 2022 }}, p. 144.</ref> It can be expressed in terms of SI base units ([[metre|m]], [[kilogram|kg]], [[second|s]], and [[ampere|A]]) as |
||
: <math alt="volt equals kilogram times meter squared per ampere per second cubed"> |
|||
\text{V} = \frac{\text{power}}{\text{electric current}} = \frac{\text{W}}{\text{A}} = \frac{\text{kg}{\cdot}\text{m}^2{\cdot}\text{s}^{-3}}{\text{A}} = \text{kg}{\cdot}\text{m}^2{\cdot}\text{s}^{-3}{\cdot}{\text{A}^{-1}}.</math> |
|||
Equivalently, it is the potential difference between two points that will impart one [[joule]] of [[energy]] per [[coulomb]] of charge that passes through it. It can be expressed in terms of SI base units ([[metre|m]], [[kilogram|kg]], [[second|s]], and [[ampere|A]]) as |
|||
: <math alt="volt equals kilogram times meter squared per ampere per second cubed"> |
: <math alt="volt equals kilogram times meter squared per ampere per second cubed"> |
||
\text{V} = \frac{\text{potential energy}}{\text{charge}} = \frac{\text{J}}{\text{C}} = \frac{\text{kg}{\cdot}\text{m}^2{\cdot}\text{s}^{-2}}{\text{A}{\cdot}\text{s}} = \text{kg}{\cdot}\text{m}^2{\cdot}\text{s}^{-3}{\cdot}{\text{A}^{-1}}.</math> |
\text{V} = \frac{\text{potential energy}}{\text{charge}} = \frac{\text{J}}{\text{C}} = \frac{\text{kg}{\cdot}\text{m}^2{\cdot}\text{s}^{-2}}{\text{A}{\cdot}\text{s}} = \text{kg}{\cdot}\text{m}^2{\cdot}\text{s}^{-3}{\cdot}{\text{A}^{-1}}.</math> |
||
It can also be expressed as amperes times [[ohm]]s (current times resistance, [[Ohm's law]]), webers per second (magnetic flux per time), watts per ampere (power per current), or joules per coulomb (energy per charge), which is also equivalent to [[electronvolt]]s per [[elementary charge]]: |
It can also be expressed as amperes times [[ohm]]s (current times resistance, [[Ohm's law]]), [[Weber (unit)|webers]] per second (magnetic flux per time), watts per ampere (power per current), or joules per coulomb (energy per charge), which is also equivalent to [[electronvolt]]s per [[elementary charge]]: |
||
: <math alt="volt equals ampere times ohm, watt per ampere, and joules per coulomb"> |
: <math alt="volt equals ampere times ohm, watt per ampere, and joules per coulomb"> |
||
\text{V} = \text{A}{\cdot}\Omega = \frac{\text{Wb}}{\text{s}} = \frac{\text{W}}{\text{A}} = \frac{\text{J}}{\text{C}} = \frac{\text{eV}}{e}.</math> |
\text{V} = \text{A}{\cdot}\Omega = \frac{\text{Wb}}{\text{s}} = \frac{\text{W}}{\text{A}} = \frac{\text{J}}{\text{C}} = \frac{\text{eV}}{e}.</math> |
||
Line 30: | Line 37: | ||
=== Josephson junction definition === |
=== Josephson junction definition === |
||
{{ |
{{Main|Josephson voltage standard}} |
||
⚫ | Historically |
||
⚫ | Historically the "[[Conventional electrical unit|conventional]]" volt, ''V''<sub>90</sub>, defined in 1987 by the 18th [[General Conference on Weights and Measures]]<ref name="cgpm-18">{{cite web|url=https://www.bipm.org/documents/20126/33145736/CGPM18.pdf/f461df63-75c1-c14d-e6b7-69867b79382f|title=Resolutions of the CGPM: 18th meeting (12–15 October 1987)|access-date=27 February 2022|archive-date=27 February 2022|archive-url=https://web.archive.org/web/20220227150143/https://www.bipm.org/documents/20126/33145736/CGPM18.pdf/f461df63-75c1-c14d-e6b7-69867b79382f|url-status=live}}</ref> and in use from 1990 to 2019, was implemented using the [[Josephson effect]] for exact frequency-to-voltage conversion, combined with the [[Caesium standard|caesium frequency standard]]. Though the Josephson effect is still used to realize a volt, the constant used has changed slightly. |
||
⚫ | For the [[Josephson constant]], ''K''<sub>J</sub> = 2''e''/''h'' (where ''e'' is the [[elementary charge]] and ''h'' is the [[Planck constant]]), a "conventional" value ''K''<sub>J-90</sub> = 0.4835979 GHz/μV was used for the purpose of defining the volt. As a consequence of the [[2019 |
||
⚫ | For the [[Magnetic flux quantum|Josephson constant]], ''K''<sub>J</sub> = 2''e''/''h'' (where ''e'' is the [[elementary charge]] and ''h'' is the [[Planck constant]]), a "conventional" value ''K''<sub>J-90</sub> = 0.4835979 GHz/μV was used for the purpose of defining the volt. As a consequence of the [[2019 revision of the SI]], as of 2019 the Josephson constant has an exact value of {{math|''K''<sub>J</sub>}} = {{val|483597.84841698|end=...|u=GHz/V}}, which replaced the conventional value ''K''<sub>J-90</sub>. |
||
⚫ | This standard is typically realized using a series-connected array of several thousand or tens of thousands of [[ |
||
⚫ | This standard is typically realized using a series-connected array of several thousand or tens of thousands of [[Electrical junction|junctions]], excited by microwave signals between 10 and 80 GHz (depending on the array design).<ref name=ieee-josephson>{{Citation |title=1 Volt DC Programmable Josephson Voltage Standard |first1=Charles J. |last1=Burroughs |first2=Samuel P. |last2=Bent |first3=Todd E. |last3=Harvey |first4=Clark A. |last4=Hamilton |journal=IEEE Transactions on Applied Superconductivity |date=1 June 1999 |volume=9 |number=3 |pages=4145–4149 |issn=1051-8223 |publisher=[[Institute of Electrical and Electronics Engineers]] (IEEE) |doi=10.1109/77.783938 |bibcode=1999ITAS....9.4145B |s2cid=12970127 |url=https://zenodo.org/record/1232191}}</ref> Empirically, several experiments have shown that the method is independent of device design, material, measurement setup, etc., and no correction terms are required in a practical implementation.<ref>{{Citation |title=Current status of the quantum metrology triangle |first=Mark W. |last=Keller |url=http://qdev.boulder.nist.gov/817.03/pubs/downloads/set/Metrologia%2045,%20102.pdf |journal=Metrologia |volume=45 |number=1 |pages=102–109 |date=18 January 2008 |issn=0026-1394 |doi=10.1088/0026-1394/45/1/014 |quote=Theoretically, there are no current predictions for any correction terms. Empirically, several experiments have shown that ''K''<sub>J</sub> and ''R''<sub>K</sub> are independent of device design, material, measurement setup, etc. This demonstration of universality is consistent with the exactness of the relations, but does not prove it outright. |bibcode=2008Metro..45..102K |s2cid=122008182 |access-date=11 April 2010 |archive-url=https://web.archive.org/web/20100527094953/http://qdev.boulder.nist.gov/817.03/pubs/downloads/set/Metrologia%2045,%20102.pdf |archive-date=27 May 2010 |url-status=dead}}</ref> |
||
== Water-flow analogy == |
== Water-flow analogy == |
||
In the ''[[hydraulic analogy|water-flow analogy]]'', sometimes used to explain electric circuits by comparing them with water-filled pipes, [[voltage]] (difference in electric potential) is likened to difference in water |
In the ''[[hydraulic analogy|water-flow analogy]]'', sometimes used to explain electric circuits by comparing them with water-filled pipes, [[voltage]] (difference in electric potential) is likened to difference in water pressure, while [[electric current|current]] is proportional to the amount of water flowing. A [[resistor]] would be a reduced diameter somewhere in the piping or something akin to a radiator offering resistance to flow. |
||
The relationship between voltage and current is defined (in ohmic devices like |
The relationship between voltage and current is defined (in ohmic devices like resistors) by [[Ohm's law]]. Ohm's Law is analogous to the [[Hagen–Poiseuille equation]], as both are linear models relating [[flux]] and [[potential]] in their respective systems. |
||
== Common voltages {{anchor|Common values}}== |
== Common voltages {{anchor|Common values}} == |
||
[[File:Electronic multi meter.jpg|thumb| A [[multimeter]] can be used to measure the voltage between two positions.]] |
[[File:Electronic multi meter.jpg|thumb| A [[multimeter]] can be used to measure the voltage between two positions.]] |
||
[[File:BateriaR14.jpg|upright|thumb|1.5 V C-cell batteries]] |
[[File:BateriaR14.jpg|upright|thumb|1.5 V C-cell batteries]] |
||
The voltage produced by each [[electrochemical cell]] in a [[ |
The voltage produced by each [[electrochemical cell]] in a [[Electric battery|battery]] is determined by the chemistry of that cell (see {{Section link|Galvanic cell|Cell voltage}}). Cells can be combined in series for multiples of that voltage, or additional circuitry added to adjust the voltage to a different level. Mechanical generators can usually be constructed to any voltage in a range of feasibility. |
||
Nominal voltages of familiar sources: |
Nominal voltages of familiar sources: |
||
* [[Nerve cell]] [[resting potential]]: ~75 mV<ref>Bullock, Orkand, and Grinnell, pp. 150–151; Junge, pp. 89–90; Schmidt-Nielsen, p. 484.</ref> |
* [[Neuron|Nerve cell]] [[resting potential]]: ~75 mV<ref>Bullock, Orkand, and Grinnell, pp. 150–151; Junge, pp. 89–90; Schmidt-Nielsen, p. 484.</ref> |
||
* Single-cell, rechargeable [[ |
* Single-cell, rechargeable [[Nickel–metal hydride battery|NiMH]]<ref>{{cite book |last1=Horowitz |first1=Paul |last2=Winfield |first2=Hill |title=The Art of Electronics |date=2015 |publisher=Cambridge Univ. Press |location=Cambridge [u.a.] |isbn=978-0-521-809269 |page=689 |edition=3.}}</ref> or [[nickel–cadmium battery|NiCd]] battery: 1.2 V |
||
* Single-cell, non-rechargeable (e.g., [[ |
* Single-cell, non-rechargeable (e.g., [[Electric battery|AAA, AA, C and D cells]]): [[alkaline battery]]: 1.5 V;<ref>{{cite web |url=http://www.ti.com/lit/an/slva194/slva194.pdf |title=Single-cell Battery Discharge Characteristics Using the TPS61070 Boost Converter |author1=SK Loo |author2=Keith Keller |publisher=Texas Instruments |date=Aug 2004 |url-status=live |archive-url=https://web.archive.org/web/20231015141242/https://www.ti.com/lit/an/slva194/slva194.pdf |archive-date= 15 October 2023}}</ref> [[zinc–carbon battery]]: 1.56 V if fresh and unused |
||
* [[ |
* [[Logic level#Logic voltage levels|Logic voltage levels]]: 1.2 V, 1.5 V, 1.8 V, 2.5 V, 3.3 V, 5.0 V |
||
* [[Lithium iron phosphate battery|LiFePO<sub>4</sub>]] rechargeable battery: 3.3 V |
* [[Lithium iron phosphate battery|LiFePO<sub>4</sub>]] rechargeable battery: 3.3 V |
||
* [[Cobalt]]-based [[lithium polymer]] rechargeable battery: 3.75 V (see [[Comparison of commercial battery types]]) |
* [[Cobalt]]-based [[Lithium polymer battery|lithium polymer]] rechargeable battery: 3.75 V (see [[Comparison of commercial battery types]]) |
||
* [[ |
* [[Transistor–transistor logic]]/[[CMOS]] (TTL) power supply: 5 V |
||
* [[USB]]: 5 V DC |
* [[USB]]: 5 V DC |
||
* [[PP3 battery]]: 9 V |
* [[Nine-volt battery|PP3 battery]]: 9 V |
||
* [[Automotive battery|Automobile battery]] systems are 2.1 volts per cell; a "12 V" battery is 6 cells, or 12.6 V; a "24 V" battery is 12 cells, or 25.2 V. Some antique vehicles use "6 V" 3-cell batteries, or 6.3 volts. |
* [[Automotive battery|Automobile battery]] systems are 2.1 volts per cell; a "12 V" battery is 6 cells, or 12.6 V; a "24 V" battery is 12 cells, or 25.2 V. Some antique vehicles use "6 V" 3-cell batteries, or 6.3 volts. |
||
* Household [[mains electricity]] AC: (see [[List of countries with mains power plugs, voltages and frequencies]]) |
* Household [[mains electricity]] AC: (see [[Mains electricity by country|List of countries with mains power plugs, voltages and frequencies]]) |
||
** 100 V in Japan |
** 100 V in Japan |
||
** 120 V in North America |
** 120 V in North America |
||
** 230 V in Europe, Asia, Africa and Australia |
** 230 V in Europe, Asia, Africa and Australia |
||
* [[Rapid transit]] [[third rail]]: 600–750 V (see [[List of railway electrification systems]]) |
* [[Rapid transit]] [[third rail]]: 600–750 V (see [[List of railway electrification systems]]) |
||
* High-speed train overhead power lines: [[25 kV AC|25 kV at 50 Hz]], but see the [[List of railway electrification systems]] and [[25 kV AC#60 Hz|25 kV at 60 Hz]] for exceptions. |
* High-speed train overhead power lines: [[25 kV AC railway electrification|25 kV at 50 Hz]], but see the [[List of railway electrification systems]] and [[25 kV AC railway electrification#25 kV AC at 60 Hz|25 kV at 60 Hz]] for exceptions. |
||
* High-voltage [[electric power transmission]] lines: 110 kV and up (1.15 MV is the record; the highest active voltage is 1.10 MV<ref>{{ |
* High-voltage [[electric power transmission]] lines: 110 kV and up (1.15 MV is the record; the highest active voltage is 1.10 MV<ref>{{cite web |url=https://www.bloomberg.com/news/articles/2019-01-02/world-s-biggest-ultra-high-voltage-line-powers-up-across-china |title=World's Biggest Ultra-High Voltage Line Powers Up Across China |website=Bloomberg |url-access=subscription |access-date=7 January 2020 |date=1 January 2019}}</ref>) |
||
* [[Lightning]]: a maximum of around 150 MV.<ref>{{cite web |url=https://www.riskva.com/fff/lightning_062613.html |author=Paul H. Risk |title=Lightning – High-Voltage Nature |website=RiskVA |date=26 |
* [[Lightning]]: a maximum of around 150 MV.<ref>{{cite web |url=https://www.riskva.com/fff/lightning_062613.html |author=Paul H. Risk |title=Lightning – High-Voltage Nature |website=RiskVA |date=26 June 2013 |access-date=23 April 2021 |archive-date=23 April 2021 |archive-url=https://web.archive.org/web/20210423220123/https://www.riskva.com/fff/lightning_062613.html |url-status=live }}</ref> |
||
== History == |
== History == |
||
Line 72: | Line 80: | ||
[[File:PSM V85 D521 Group photograph of herman helmholtz and academic friends.png|thumb|Group photograph of [[Hermann von Helmholtz|Hermann Helmholtz]], his wife (seated) and academic friends [[Hugo Kronecker]] (left), [[Thomas Corwin Mendenhall]] (right), [[Henry Villard]] (center) during the International Electrical Congress]] |
[[File:PSM V85 D521 Group photograph of herman helmholtz and academic friends.png|thumb|Group photograph of [[Hermann von Helmholtz|Hermann Helmholtz]], his wife (seated) and academic friends [[Hugo Kronecker]] (left), [[Thomas Corwin Mendenhall]] (right), [[Henry Villard]] (center) during the International Electrical Congress]] |
||
In 1800, as the result of a professional disagreement over the galvanic response advocated by [[Luigi Galvani]], [[Alessandro Volta]] developed the so-called [[voltaic pile]], a forerunner of the [[ |
In 1800, as the result of a professional disagreement over the galvanic response advocated by [[Luigi Galvani]], [[Alessandro Volta]] developed the so-called [[voltaic pile]], a forerunner of the [[Electric battery|battery]], which produced a steady electric [[Electric current|current]]. Volta had determined that the most effective pair of dissimilar metals to produce electricity was [[zinc]] and [[silver]]. In 1861, [[Josiah Latimer Clark|Latimer Clark]] and Sir [[Charles Tilston Bright|Charles Bright]] coined the name "volt" for the unit of resistance.<ref>As names for units of various electrical quantities, Bright and Clark suggested "ohma" for voltage, "farad" for charge, "galvat" for current, and "volt" for resistance. See: |
||
* Latimer Clark and Sir Charles Bright (1861) [https://www.biodiversitylibrary.org/item/93052#page/483/mode/1up "On the formation of standards of electrical quantity and resistance"], ''Report of the Thirty-first Meeting of the British Association for the Advancement of Science'' (Manchester, England: |
* Latimer Clark and Sir Charles Bright (1861) [https://www.biodiversitylibrary.org/item/93052#page/483/mode/1up "On the formation of standards of electrical quantity and resistance"] {{Webarchive|url=https://web.archive.org/web/20121108105352/http://www.biodiversitylibrary.org/item/93052#page/483/mode/1up |date=8 November 2012 }}, ''Report of the Thirty-first Meeting of the British Association for the Advancement of Science'' (Manchester, England: September 1861), section: Mathematics and Physics, pp. 37–38. |
||
* Latimer Clark and Sir Charles Bright (November |
* Latimer Clark and Sir Charles Bright (9 November 1861) [https://babel.hathitrust.org/cgi/pt?id=nyp.33433090837166;view=1up;seq=15 "Measurement of electrical quantities and resistance"], ''The Electrician'', '''1''' (1): 3–4.</ref> By 1873, the British Association for the Advancement of Science had defined the volt, ohm, and farad.<ref>Sir W. Thomson, et al. (1873) [https://www.biodiversitylibrary.org/page/29853513#page/324/mode/1up "First report of the Committee for the Selection and Nomenclature of Dynamical and Electrical Units"] {{Webarchive|url=https://web.archive.org/web/20170423152619/http://www.biodiversitylibrary.org/page/29853513#page/324/mode/1up |date=23 April 2017 }}, ''Report of the 43rd Meeting of the British Association for the Advancement of Science'' (Bradford, September 1873), pp. 222–225. From p. 223: "The "ohm," as represented by the original standard coil, is approximately 10<sup>9</sup> C.G.S. units of resistance; the "volt" is approximately 10<sup>8</sup> C.G.S. units of electromotive force; and the "farad" is approximately 1/10<sup>9</sup> of the C.G.S. unit of capacity."</ref> In 1881, the International Electrical Congress, now the [[International Electrotechnical Commission]] (IEC), approved the volt as the unit for electromotive force.<ref>(Anon.) (24 September 1881) [https://babel.hathitrust.org/cgi/pt?id=nyp.33433090837489;view=1up;seq=309 "The Electrical Congress"] {{Webarchive|url=https://web.archive.org/web/20190306002556/https://babel.hathitrust.org/cgi/pt?id=nyp.33433090837489;view=1up;seq=309 |date=6 March 2019 }}, ''The Electrician'', '''7''': 297.</ref> They made the volt equal to 10<sup>8</sup> [[Centimetre–gram–second system of units|cgs units]] of voltage, the cgs system at the time being the customary system of units in science. They chose such a ratio because the cgs unit of voltage is inconveniently small and one volt in this definition is approximately the emf of a [[Daniell cell]], the standard source of voltage in the telegraph systems of the day.<ref name=Hamer>{{cite book |title=Standard Cells: Their Construction, Maintenance, and Characteristics |publisher=US National Bureau of Standards |last=Hamer |first=Walter J. |date=15 January 1965 |series=National Bureau of Standards Monograph #84 |url=https://www.nist.gov/calibrations/upload/mn84.pdf |access-date=13 July 2017 |archive-date=3 March 2016 |archive-url=https://web.archive.org/web/20160303203423/http://www.nist.gov/calibrations/upload/mn84.pdf |url-status=live }}</ref> At that time, the volt was defined as the potential difference [i.e., what is nowadays called the "voltage (difference)"] across a conductor when a current of one [[ampere]] dissipates one [[watt]] of power. |
||
The "international volt" was defined in 1893 as |
The "international volt" was defined in 1893 as {{fraction|1.434}} of the [[Electromotive force|emf]] of a [[Clark cell]]. This definition was abandoned in 1908 in favor of a definition based on the international [[ohm]] and international ampere until the entire set of "reproducible units" was abandoned in 1948.<ref name=BLR47.12>{{cite journal |date=December 1947 |title=Revised Values for Electrical Units |journal= Bell Laboratories Record |volume=XXV |issue=12 |pages=441 |url=http://www.americanradiohistory.com/Archive-Bell-Laboratories-Record/40s/Bell-Laboratories-Record-1947-12.pdf}}</ref> |
||
A [[2019 |
A [[2019 revision of the SI]], including defining the value of the [[elementary charge]], took effect on 20 May 2019.<ref name=draft-resolution-A>{{Citation |title=Draft Resolution A "On the revision of the International System of units (SI)" to be submitted to the CGPM at its 26th meeting (2018) |url=https://www.bipm.org/utils/en/pdf/CGPM/Draft-Resolution-A-EN.pdf |access-date=2 November 2018 |archive-date=29 April 2018 |archive-url=https://web.archive.org/web/20180429025229/https://www.bipm.org/utils/en/pdf/CGPM/Draft-Resolution-A-EN.pdf |url-status=dead}}</ref> |
||
|title=Draft Resolution A "On the revision of the International System of units (SI)" to be submitted to the CGPM at its 26th meeting (2018) |
|||
|url=https://www.bipm.org/utils/en/pdf/CGPM/Draft-Resolution-A-EN.pdf |
|||
|access-date=2018-11-02 |
|||
|archive-date=2018-04-29 |
|||
|archive-url=https://web.archive.org/web/20180429025229/https://www.bipm.org/utils/en/pdf/CGPM/Draft-Resolution-A-EN.pdf |
|||
|url-status=dead |
|||
}}</ref> |
|||
== See also == |
== See also == |
||
{{Portal|Energy}} |
{{Portal|Energy}} |
||
{{div col|colwidth=24em}} |
{{div col|colwidth=24em}} |
||
* [[Orders of magnitude (voltage)]] |
* [[Orders of magnitude (voltage)]] |
||
* [[List of railway electrification systems|Rail traction voltage]] |
* [[List of railway electrification systems|Rail traction voltage]] |
||
* [[SI electromagnetism units]] |
* [[SI electromagnetism units]] |
||
* [[SI prefix]] for unit prefixes |
* [[Metric prefix#List of SI prefixes|SI prefix]] for unit prefixes |
||
* [[Railway electrification |
* [[Railway electrification#Standardised voltages|Standardised railway voltages]] |
||
* [[Voltmeter]] |
* [[Voltmeter]] |
||
{{div col end}} |
{{div col end}} |
||
== References == |
== References == |
||
{{Reflist| |
{{Reflist|2}} |
||
== External links == |
== External links == |
Latest revision as of 00:05, 9 December 2024
This article needs to be updated.(November 2024) |
volt | |
---|---|
General information | |
Unit system | SI |
Unit of | electric potential, electromotive force |
Symbol | V |
Named after | Alessandro Volta |
SI base units | kg⋅m2⋅s−3⋅A−1 |
The volt (symbol: V) is the unit of electric potential, electric potential difference (voltage), and electromotive force in the International System of Units (SI).[1]
Definition
[edit]One volt is defined as the electric potential between two points of a conducting wire when an electric current of one ampere dissipates one watt of power between those points.[2] It can be expressed in terms of SI base units (m, kg, s, and A) as
Equivalently, it is the potential difference between two points that will impart one joule of energy per coulomb of charge that passes through it. It can be expressed in terms of SI base units (m, kg, s, and A) as
It can also be expressed as amperes times ohms (current times resistance, Ohm's law), webers per second (magnetic flux per time), watts per ampere (power per current), or joules per coulomb (energy per charge), which is also equivalent to electronvolts per elementary charge:
The volt is named after Alessandro Volta. As with every SI unit named for a person, its symbol starts with an upper case letter (V), but when written in full, it follows the rules for capitalisation of a common noun; i.e., volt becomes capitalised at the beginning of a sentence and in titles but is otherwise in lower case.
Josephson junction definition
[edit]Historically the "conventional" volt, V90, defined in 1987 by the 18th General Conference on Weights and Measures[3] and in use from 1990 to 2019, was implemented using the Josephson effect for exact frequency-to-voltage conversion, combined with the caesium frequency standard. Though the Josephson effect is still used to realize a volt, the constant used has changed slightly.
For the Josephson constant, KJ = 2e/h (where e is the elementary charge and h is the Planck constant), a "conventional" value KJ-90 = 0.4835979 GHz/μV was used for the purpose of defining the volt. As a consequence of the 2019 revision of the SI, as of 2019 the Josephson constant has an exact value of KJ = 483597.84841698... GHz/V, which replaced the conventional value KJ-90.
This standard is typically realized using a series-connected array of several thousand or tens of thousands of junctions, excited by microwave signals between 10 and 80 GHz (depending on the array design).[4] Empirically, several experiments have shown that the method is independent of device design, material, measurement setup, etc., and no correction terms are required in a practical implementation.[5]
Water-flow analogy
[edit]In the water-flow analogy, sometimes used to explain electric circuits by comparing them with water-filled pipes, voltage (difference in electric potential) is likened to difference in water pressure, while current is proportional to the amount of water flowing. A resistor would be a reduced diameter somewhere in the piping or something akin to a radiator offering resistance to flow.
The relationship between voltage and current is defined (in ohmic devices like resistors) by Ohm's law. Ohm's Law is analogous to the Hagen–Poiseuille equation, as both are linear models relating flux and potential in their respective systems.
Common voltages
[edit]The voltage produced by each electrochemical cell in a battery is determined by the chemistry of that cell (see Galvanic cell § Cell voltage). Cells can be combined in series for multiples of that voltage, or additional circuitry added to adjust the voltage to a different level. Mechanical generators can usually be constructed to any voltage in a range of feasibility.
Nominal voltages of familiar sources:
- Nerve cell resting potential: ~75 mV[6]
- Single-cell, rechargeable NiMH[7] or NiCd battery: 1.2 V
- Single-cell, non-rechargeable (e.g., AAA, AA, C and D cells): alkaline battery: 1.5 V;[8] zinc–carbon battery: 1.56 V if fresh and unused
- Logic voltage levels: 1.2 V, 1.5 V, 1.8 V, 2.5 V, 3.3 V, 5.0 V
- LiFePO4 rechargeable battery: 3.3 V
- Cobalt-based lithium polymer rechargeable battery: 3.75 V (see Comparison of commercial battery types)
- Transistor–transistor logic/CMOS (TTL) power supply: 5 V
- USB: 5 V DC
- PP3 battery: 9 V
- Automobile battery systems are 2.1 volts per cell; a "12 V" battery is 6 cells, or 12.6 V; a "24 V" battery is 12 cells, or 25.2 V. Some antique vehicles use "6 V" 3-cell batteries, or 6.3 volts.
- Household mains electricity AC: (see List of countries with mains power plugs, voltages and frequencies)
- 100 V in Japan
- 120 V in North America
- 230 V in Europe, Asia, Africa and Australia
- Rapid transit third rail: 600–750 V (see List of railway electrification systems)
- High-speed train overhead power lines: 25 kV at 50 Hz, but see the List of railway electrification systems and 25 kV at 60 Hz for exceptions.
- High-voltage electric power transmission lines: 110 kV and up (1.15 MV is the record; the highest active voltage is 1.10 MV[9])
- Lightning: a maximum of around 150 MV.[10]
History
[edit]In 1800, as the result of a professional disagreement over the galvanic response advocated by Luigi Galvani, Alessandro Volta developed the so-called voltaic pile, a forerunner of the battery, which produced a steady electric current. Volta had determined that the most effective pair of dissimilar metals to produce electricity was zinc and silver. In 1861, Latimer Clark and Sir Charles Bright coined the name "volt" for the unit of resistance.[11] By 1873, the British Association for the Advancement of Science had defined the volt, ohm, and farad.[12] In 1881, the International Electrical Congress, now the International Electrotechnical Commission (IEC), approved the volt as the unit for electromotive force.[13] They made the volt equal to 108 cgs units of voltage, the cgs system at the time being the customary system of units in science. They chose such a ratio because the cgs unit of voltage is inconveniently small and one volt in this definition is approximately the emf of a Daniell cell, the standard source of voltage in the telegraph systems of the day.[14] At that time, the volt was defined as the potential difference [i.e., what is nowadays called the "voltage (difference)"] across a conductor when a current of one ampere dissipates one watt of power.
The "international volt" was defined in 1893 as 1⁄1.434 of the emf of a Clark cell. This definition was abandoned in 1908 in favor of a definition based on the international ohm and international ampere until the entire set of "reproducible units" was abandoned in 1948.[15]
A 2019 revision of the SI, including defining the value of the elementary charge, took effect on 20 May 2019.[16]
See also
[edit]References
[edit]- ^ "SI Brochure, Table 3 (Section 2.2.2)". BIPM. 2006. Archived from the original on 18 June 2007. Retrieved 29 July 2007.
- ^ BIPM SI Brochure: Appendix 1 Archived 27 February 2022 at the Wayback Machine, p. 144.
- ^ "Resolutions of the CGPM: 18th meeting (12–15 October 1987)". Archived from the original on 27 February 2022. Retrieved 27 February 2022.
- ^ Burroughs, Charles J.; Bent, Samuel P.; Harvey, Todd E.; Hamilton, Clark A. (1 June 1999), "1 Volt DC Programmable Josephson Voltage Standard", IEEE Transactions on Applied Superconductivity, 9 (3), Institute of Electrical and Electronics Engineers (IEEE): 4145–4149, Bibcode:1999ITAS....9.4145B, doi:10.1109/77.783938, ISSN 1051-8223, S2CID 12970127
- ^ Keller, Mark W. (18 January 2008), "Current status of the quantum metrology triangle" (PDF), Metrologia, 45 (1): 102–109, Bibcode:2008Metro..45..102K, doi:10.1088/0026-1394/45/1/014, ISSN 0026-1394, S2CID 122008182, archived from the original (PDF) on 27 May 2010, retrieved 11 April 2010,
Theoretically, there are no current predictions for any correction terms. Empirically, several experiments have shown that KJ and RK are independent of device design, material, measurement setup, etc. This demonstration of universality is consistent with the exactness of the relations, but does not prove it outright.
- ^ Bullock, Orkand, and Grinnell, pp. 150–151; Junge, pp. 89–90; Schmidt-Nielsen, p. 484.
- ^ Horowitz, Paul; Winfield, Hill (2015). The Art of Electronics (3. ed.). Cambridge [u.a.]: Cambridge Univ. Press. p. 689. ISBN 978-0-521-809269.
- ^ SK Loo; Keith Keller (August 2004). "Single-cell Battery Discharge Characteristics Using the TPS61070 Boost Converter" (PDF). Texas Instruments. Archived (PDF) from the original on 15 October 2023.
- ^ "World's Biggest Ultra-High Voltage Line Powers Up Across China". Bloomberg. 1 January 2019. Retrieved 7 January 2020.
- ^ Paul H. Risk (26 June 2013). "Lightning – High-Voltage Nature". RiskVA. Archived from the original on 23 April 2021. Retrieved 23 April 2021.
- ^ As names for units of various electrical quantities, Bright and Clark suggested "ohma" for voltage, "farad" for charge, "galvat" for current, and "volt" for resistance. See:
- Latimer Clark and Sir Charles Bright (1861) "On the formation of standards of electrical quantity and resistance" Archived 8 November 2012 at the Wayback Machine, Report of the Thirty-first Meeting of the British Association for the Advancement of Science (Manchester, England: September 1861), section: Mathematics and Physics, pp. 37–38.
- Latimer Clark and Sir Charles Bright (9 November 1861) "Measurement of electrical quantities and resistance", The Electrician, 1 (1): 3–4.
- ^ Sir W. Thomson, et al. (1873) "First report of the Committee for the Selection and Nomenclature of Dynamical and Electrical Units" Archived 23 April 2017 at the Wayback Machine, Report of the 43rd Meeting of the British Association for the Advancement of Science (Bradford, September 1873), pp. 222–225. From p. 223: "The "ohm," as represented by the original standard coil, is approximately 109 C.G.S. units of resistance; the "volt" is approximately 108 C.G.S. units of electromotive force; and the "farad" is approximately 1/109 of the C.G.S. unit of capacity."
- ^ (Anon.) (24 September 1881) "The Electrical Congress" Archived 6 March 2019 at the Wayback Machine, The Electrician, 7: 297.
- ^ Hamer, Walter J. (15 January 1965). Standard Cells: Their Construction, Maintenance, and Characteristics (PDF). National Bureau of Standards Monograph #84. US National Bureau of Standards. Archived (PDF) from the original on 3 March 2016. Retrieved 13 July 2017.
- ^ "Revised Values for Electrical Units" (PDF). Bell Laboratories Record. XXV (12): 441. December 1947.
- ^ Draft Resolution A "On the revision of the International System of units (SI)" to be submitted to the CGPM at its 26th meeting (2018) (PDF), archived from the original (PDF) on 29 April 2018, retrieved 2 November 2018