quantitykind:ElectricCurrentPhasor

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

Type
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.

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:comment
Applicable units are those of quantitykind:ElectricCurrentPhasor
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.
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#" > 
  <rdf:Description rdf:about="http://qudt.org/vocab/quantitykind/ElectricCurrentPhasor">
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/AttoA"/>
    <rdfs:comment>Applicable units are those of quantitykind:ElectricCurrentPhasor</rdfs:comment>
    <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>
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    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/TeraA"/>
    <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:informativeReference rdf:datatype="http://www.w3.org/2001/XMLSchema#anyURI">http://en.wikipedia.org/wiki/Phasor_(electronics)</j.0:informativeReference>
    <j.1:description rdf:datatype="http://qudt.org/schema/qudt/LatexString">"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.1:description>
    <rdf:type rdf:resource="http://qudt.org/schema/qudt/QuantityKind"/>
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    <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>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/GigaA"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/FemtoA"/>
    <j.0:latexSymbol rdf:datatype="http://qudt.org/schema/qudt/LatexString">$\underline{I}$</j.0:latexSymbol>
  </rdf:Description>
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TURTLE
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<http://qudt.org/vocab/quantitykind/ElectricCurrentPhasor>
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  <http://qudt.org/schema/qudt/informativeReference> "http://en.wikipedia.org/wiki/Phasor_(electronics)"^^xsd:anyURI ;
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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:comment "Applicable units are those of quantitykind:ElectricCurrentPhasor" ;
  rdfs:isDefinedBy <http://qudt.org/2.1/vocab/quantitykind> ;
  rdfs:label "Electric Current Phasor"@en ;
.
JSON
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    ,"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." 
    ,"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." 
    ,"has dimension vector":"dimension:A0E1L0I0M0H0T0D0" 
    ,"informative reference":"http:\/\/en.wikipedia.org\/wiki\/Phasor_(electronics)" 
    ,"informative reference":"http:\/\/www.electropedia.org\/iev\/iev.nsf\/display?openform&amp;ievref=131-11-26" 
    ,"informative reference":"http:\/\/www.iso.org\/iso\/home\/store\/catalogue_tc\/catalogue_detail.htm?csnumber=31891" 
    ,"isDefinedBy":"&lt;http:\/\/qudt.org\/2.1\/vocab\/quantitykind&gt;" 
    ,"label":"Electric Current Phasor" 
    ,"latex definition":"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 $\\underline{I} = Ie^{ja}$." 
    ,"latex symbol":"$\\underline{I}$" 
    ,"type":"qudt:QuantityKind" 
    ]}
JSON-LD
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  "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.",
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