quantitykind:ElectricPotentialqudt:QuantityKind| Predicate | Object |
|---|---|
rdf:type |
qudt:QuantityKind |
dcterms:description |
The Electric Potential is a scalar valued quantity associated with an electric field. The electric potential \(\phi(x)\) at a point, \(x\), is formally defined as the line integral of the electric field taken along a path from x to the point at infinity. If the electric field is static, that is time independent, then the choice of the path is arbitrary; however if the electric field is time dependent, taking the integral a different paths will produce different results. |
qudt:applicableUnit |
|
qudt:exactMatch |
|
qudt:hasDimensionVector |
qkdv:A0E-1L2I0M1H0T-3D0 |
qudt:informativeReference |
http://www.iso.org/iso/home/store/catalogue_tc/catalogue_detail.htm?csnumber=31891 |
qudt:isoNormativeReference |
http://www.iso.org/iso/catalogue_detail?csnumber=43012 |
qudt:latexDefinition |
\(-\text{grad} \; V = E + \frac{\partial A}{\partial t}\), where \(E\) is electric field strength, \(A\) is magentic vector potential and \(t\) is time. |
qudt:latexSymbol |
\(\phi\) |
qudt:symbol |
“V” |
qudt:wikidataMatch |
http://www.wikidata.org/entity/Q55451 |
rdfs:comment |
“Applicable units are those of quantitykind:ElectricPotential” |
rdfs:isDefinedBy |
http://qudt.org/3.1.11/vocab/quantitykind |
rdfs:label |
Show 22 values
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skos:altLabel |
“vis electromotrix”@la |