
thumb|An example of series RLC circuit and respective phasor diagram for a specific . The arrows in the upper diagram are phasors, drawn in a phasor diagram ([[complex plane without axis shown), which must not be confused with the arrows in the lower diagram, which are the reference polarity for the voltages and the reference direction for the current.]]
thumb|An example of series RLC circuit and respective phasor diagram for a specific . The arrows in the upper diagram are phasors, drawn in a phasor diagram ([[complex plane without axis shown), which must not be confused with the arrows in the lower diagram, which are the reference polarity for the voltages and the reference direction for the current.]]
In physics and engineering, a phasor (a portmanteau of phase vector) is a complex number representing a sinusoidal function whose amplitude and initial phase are time-invariant and whose angular frequency is fixed. It is related to a more general concept called analytic representation, which decomposes a sinusoid into the product of a complex constant and a factor depending on time and frequency. The complex constant, which depends on amplitude and phase, is known as a phasor, or complex amplitude, and (in older texts) sinor or even complexor.
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