crossman
Senior Member
- Location
- Southeast Texas
I am just now realizing it, but there is a difference between a vector and a phasor. Would someone give me the "idiot's guide" view of this?
Thanks!
Thanks!
Steve, there is something wrong here:Originally posted by steve66:
Imagine the blue phasor is our voltage:
V*e^jwt
If that voltage is applied to a linear AC circuit with passive elements, the current will also be sinusoidal, and can be represented by the phasor:
I*e^jwt+x
where x is the phase angle of the current with respect to the impedence.
It is easy to imagine the current phasor rotating with the voltage phasor, maybe lagging it by 30 deg. for example. And it is easy to imagine the projection of the real current onto the x axis.
If you imagine the two phasors rotating in sync, it is obvious that the current and voltage are related by a simple function.
If we take the voltage phasor, and divide by the current phasor, we get:
(V*e^jwt )/(I*e^jwt+x) = (V/I)e^(jwt-(jwt+x))
=(V/I)e^(-x)
Notice that this phasor doesn't rotate (the jwt has canceled out). It only has a magnitude and a phase angle.
Some are claiming we can NOT call that phasor impedence
IMO the term RMS can only be used to describe a value that varies in magnitude and alternates in polarity, namely, AC voltage or current.I am assuming that Power factor, vars, volt-amps, and reactance as defined for use with AC sine wave voltages are RMS quantities.
Right, that's the term I should have used."RMS" refers to a sinusoidal current or voltage. Right?
I've never seen it used for DC. The term "Average Value" is used for the pulsating DC output of a rectifier.you could compute an RMS value for any periodic funtion, even fluctuating DC,