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quantitykind:ElectricCurrentPhasor

http://qudt.org/vocab/quantitykind/ElectricCurrentPhasor
Types: qudt:QuantityKind
PredicateObject
rdf:type qudt:QuantityKind
dcterms:description “"Electric Current Phasor" is a representation of current as a sinusoidal integral quantity using a complex quantity whose argument is equal to the initial phase and whose modulus is equal to the root-mean-square value. A phasor is a constant complex number, usually expressed in exponential form, representing the complex amplitude (magnitude and phase) of a sinusoidal function of time. Phasors are used by electrical engineers to simplify computations involving sinusoids, where they can often reduce a differential equation problem to an algebraic one.”
qudt:applicableUnit
qudt:hasDimensionVector qkdv:A0E1L0I0M0H0T0D0
qudt:informativeReference
qudt:latexDefinition When \(i = \hat{I} \cos{(\omega t + \alpha)}\), where \(i\) is the electric current, \(\omega\) is angular frequence, \(t\) is time, and \(\alpha\) is initial phase, then \(\underline{I} = Ie^{ja}\).
qudt:latexSymbol \(\underline{I}\)
qudt:organizedUnder quantitykind:ElectricCurrent
qudt:plainTextDescription “"Electric Current Phasor" is a representation of current as a sinusoidal integral quantity using a complex quantity whose argument is equal to the initial phase and whose modulus is equal to the root-mean-square value. A phasor is a constant complex number, usually expressed in exponential form, representing the complex amplitude (magnitude and phase) of a sinusoidal function of time. Phasors are used by electrical engineers to simplify computations involving sinusoids, where they can often reduce a differential equation problem to an algebraic one. ”
qudt:wikidataMatch http://www.wikidata.org/entity/Q78514596
rdfs:comment “Applicable units are those of quantitykind:ElectricCurrentPhasor”
rdfs:isDefinedBy http://qudt.org/3.4.0/vocab/quantitykind
rdfs:label “Electric Current Phasor”@en
skos:broader quantitykind:ElectricCurrent
Generated 2026-06-25T12:40:06.344+00:00