Volt

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The volt (symbol: V) is the unit of electric potential, electric potential difference (voltage), and electromotive force in the International System of Units (SI).<ref>{{#invoke:citation/CS1|citation |CitationClass=web }}</ref>

DefinitionEdit

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.<ref>BIPM SI Brochure: Appendix 1 Template:Webarchive, p. 144.</ref> It can be expressed in terms of SI base units (m, kg, s, and 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 (m, kg, s, and A) as

<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>

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:

<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>

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Josephson junction definitionEdit

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Historically the "conventional" volt, V90, defined in 1987 by the 18th General Conference on Weights and Measures<ref name="cgpm-18">{{#invoke:citation/CS1|citation |CitationClass=web }}</ref> 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 = Template:Val 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 Template:Math = Template:Val, 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).<ref name=ieee-josephson>Template:Citation</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>Template:Citation</ref>

Water-flow analogyEdit

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

File:Electronic multi meter.jpg
A multimeter can be used to measure the voltage between two positions.
File:BateriaR14.jpg
1.5 V C-cell batteries

The voltage produced by each electrochemical cell in a battery is determined by the chemistry of that cell (see Template:Section link). 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:

|CitationClass=web }}</ref> zinc–carbon battery: 1.56 V if fresh and unused

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  • Lightning: a maximum of around 150 MV.<ref>{{#invoke:citation/CS1|citation

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HistoryEdit

File:PSM V85 D521 Group photograph of herman helmholtz and academic friends.png
Group photograph of 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 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.<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) "On the formation of standards of electrical quantity and resistance" Template:Webarchive, 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.</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) "First report of the Committee for the Selection and Nomenclature of Dynamical and Electrical Units" Template:Webarchive, 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."</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) "The Electrical Congress" Template:Webarchive, The Electrician, 7: 297.</ref> 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.<ref name=Hamer>Template:Cite book</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 Template:Fraction 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.<ref name=BLR47.12>Template:Cite journal</ref>

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>Template:Citation</ref>

See alsoEdit

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ReferencesEdit

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External linksEdit

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