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Electric Current Phasor

Applicable units are those of quantitykind:ElectricCurrentPhasor

"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.

http://www.iso.org/iso/home/store/catalogue_tc/catalogue_detail.htm?csnumber=31891

http://en.wikipedia.org/wiki/Phasor_(electronics)

http://www.electropedia.org/iev/iev.nsf/display?openform&ievref=131-11-26

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 $\underline{I} = Ie^{ja}$.

$\underline{I}$

"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.