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: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/3.1.10/vocab/quantitykind |
rdfs:label |
“Electric Current Phasor”@en |
