quantitykind:ElectricCurrentPhasor

URI: http://qudt.org/vocab/quantitykind/ElectricCurrentPhasor

Type
Description

Properties
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: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
\(\underline{I}\)
Annotations
rdfs:label
Electric Current Phasor(en)
View as:  CSV

Work in progress

RDF/XML
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    xmlns:xsd="http://www.w3.org/2001/XMLSchema#" > 
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    <rdfs:label xml:lang="en">Electric Current Phasor</rdfs:label>
    <j.0: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.</j.0:plainTextDescription>
    <j.0:latexDefinition rdf:datatype="http://qudt.org/schema/qudt/LatexString">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 \(\underline{I} = Ie^{ja}\).</j.0:latexDefinition>
    <j.0:informativeReference rdf:datatype="http://www.w3.org/2001/XMLSchema#anyURI">http://en.wikipedia.org/wiki/Phasor_(electronics)</j.0:informativeReference>
    <j.0:latexSymbol rdf:datatype="http://qudt.org/schema/qudt/LatexString">\(\underline{I}\)</j.0:latexSymbol>
    <rdf:type rdf:resource="http://qudt.org/schema/qudt/QuantityKind"/>
    <j.0:informativeReference rdf:datatype="http://www.w3.org/2001/XMLSchema#anyURI">http://www.electropedia.org/iev/iev.nsf/display?openform&amp;ievref=131-11-26</j.0:informativeReference>
    <j.0:informativeReference rdf:datatype="http://www.w3.org/2001/XMLSchema#anyURI">http://www.iso.org/iso/home/store/catalogue_tc/catalogue_detail.htm?csnumber=31891</j.0:informativeReference>
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TURTLE
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  <http://qudt.org/schema/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}\\)."^^<http://qudt.org/schema/qudt/LatexString> ;
  <http://qudt.org/schema/qudt/latexSymbol> "\\(\\underline{I}\\)"^^<http://qudt.org/schema/qudt/LatexString> ;
  <http://qudt.org/schema/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." ;
  rdfs:isDefinedBy <http://qudt.org/2.1/vocab/quantitykind> ;
  rdfs:label "Electric Current Phasor"@en ;
.
JSON
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 ,"uri":"http:\/\/qudt.org\/vocab\/quantitykind\/ElectricCurrentPhasor" 
 ,"properties":["applicable unit":"unit:A" 
    ,"description (plain text)":"\"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." 
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    ,"isDefinedBy":"&lt;http:\/\/qudt.org\/2.1\/vocab\/quantitykind&gt;" 
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    ,"latex symbol":"\\(\\underline{I}\\)" 
    ,"type":"qudt:QuantityKind" 
    ]}
JSON-LD
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