Phasor representation of AC voltage and current

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SUMMARY

The discussion focuses on the phasor representation of alternating current (AC) voltage and current, specifically detailing the relationships between RMS values and their corresponding phasor forms. It establishes that the voltage V is represented as 100∠30° V and the current I as 5∠0° A, leading to expressions for instantaneous voltage and current. The average power P is calculated using the formula P = VrmsIrms cos(θ - φ), while the reactive power Q and apparent power S are also defined, emphasizing the importance of the power factor in AC systems.

PREREQUISITES
  • Understanding of AC circuit theory
  • Familiarity with phasor notation and complex numbers
  • Knowledge of RMS (Root Mean Square) calculations
  • Basic principles of power in electrical systems
NEXT STEPS
  • Study the relationship between Vmax and Vrms in AC circuits
  • Learn about the calculation of instantaneous power in AC systems
  • Explore the concept of power factor and its significance in electrical engineering
  • Investigate the use of complex power in AC circuit analysis
USEFUL FOR

Electrical engineers, students studying AC circuit theory, and professionals involved in power system analysis will benefit from this discussion on phasor representation and power calculations in AC systems.

Astronuc
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Phasor representation of AC voltage and current.

I\,=\,5\angle{0^o}\,=\,5\,+\,j0\,A

V\,=\,100\angle{30^o}\,=\,86.6\,+\,j50\,V


in general

V\,=\,A\angle{\theta^o}\,=\,A cos{\theta}\,+\,jA sin{\theta}\,V

and similarly for I


It is assumed that the angular frequency \omega is the same throughout the system, and it is assumed that the Voltage and Current are RMS values.

For the above phasor values, the voltage and current are:

v(t) = 141.4 cos (\omegat + 30°)

and

i(t) = 7.07 cos \omegat
 
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AC Power in Phasor Form

p(t)\,=\,[V_{max}\,cos(\omega{t}+\theta)] \times [I_{max}\,cos(\omega{t}+\phi)]

becomes

p(t)\,=\,\frac{V_{max}I_{max}}{2}[cos(\theta-\phi)\,+\,cos(2\omega{t}+\theta+\phi)]

The average power is

P\,=\,V_{rms}I_{rms}\,cos(\theta-\phi)


In phasor notation,

v\,=\,V_{rms}\angle\theta

i\,=\,I_{rms}\angle\phi

but

P\,\neq\,V_{rms}I_{rms}\angle(\theta+\phi)

Instead

P\,=\,Re\{VI^*\}

and

V\,I^*\,=\,(V_{rms}\angle\theta)\times(I_{rms}\angle-\phi)

\,=\,V_{rms}I_{rms}\angle(\theta-\phi)

The real part of power is given by

P\,=\,V_{rms}I_{rms}cos(\theta-\phi)

and the reactive or imaginary part of power is

Q\,=\,V_{rms}I_{rms}sin(\theta-\phi)

and the quantity cos(\theta-\phi) is known as the power factor.

The apparent power, S, expressed as volt-amperes (VA) is given by

S (volt-amps) = P (Watts) + jQ (volt-amps-reactive) = VI*

|S|2 = |P|2 + |Q|2 = Vrms2 Irms2

PF = |P|/|S|

VAR is commonly used as a unit for "volt-amperes-reactive"

Some useful background on AC power and phasors.

http://hyperphysics.phy-astr.gsu.edu/hbase/electric/phase.html

http://www.physclips.unsw.edu.au/jw/AC.html

http://www.walter-fendt.de/ph11e/accircuit.htm
 
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phasor representation

so Phasor representation of an AC voltage is what magnitude? RMS
 
you might want to explicitly relate Vmax to Vrms and similar for the currents. in fact, Astronuc, i might define the sinusoids as

v(t) \triangleq V_{max} cos(\omega t + \theta) = \sqrt{2} V_{rms} cos(\omega t + \theta)

and

i(t) \triangleq I_{max} cos(\omega t + \phi) = \sqrt{2} I_{rms} cos(\omega t + \phi)

and then crank out the instantaneous and mean power as you did.

i dunno. just a suggestion.
 

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