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Derivation and phasor diagram of complex power

Short answer

Complex power S = VI* = P + jQ, with P = |V||I|cosφ (real power, W) and Q = |V||I|sinφ (reactive power, var). P does useful work; Q is energy exchanged with magnetic/electric fields and sets voltage levels.

Starting from voltage and current phasors, derive the expression for complex power. Construct the phasor diagram of complex power and explain the significance of the components.

Complex power S is the phasor product of the voltage and the conjugate of the current. Its real part is the average (active) power and its imaginary part is the reactive power.

Derivation

Let the instantaneous voltage and current be

v=Vmcos⁡(ωt+θv),i=Imcos⁡(ωt+θi)v = V_m\cos(\omega t + \theta_v), \qquad i = I_m\cos(\omega t + \theta_i)

The instantaneous power is

p=vi=VmIm2[cos⁡(θv−θi)+cos⁡(2ωt+θv+θi)]=∣V∣∣I∣cos⁡ϕ [1+cos⁡2(ωt+θv)]+∣V∣∣I∣sin⁡ϕ sin⁡2(ωt+θv)\begin{aligned} p = vi &= \frac{V_mI_m}{2}\left[\cos(\theta_v - \theta_i) + \cos(2\omega t + \theta_v + \theta_i)\right]\\ &= |V||I|\cos\phi\,[1 + \cos 2(\omega t + \theta_v)] + |V||I|\sin\phi\,\sin 2(\omega t + \theta_v) \end{aligned}

Here ∣V∣=Vm/2|V| = V_m/\sqrt2, ∣I∣=Im/2|I| = I_m/\sqrt2 and ϕ=θv−θi\phi = \theta_v - \theta_i.

  • The first term has average P=∣V∣∣I∣cos⁡ϕP = |V||I|\cos\phi. This is the active power.
  • The second term has zero average and peak Q=∣V∣∣I∣sin⁡ϕQ = |V||I|\sin\phi. This is the reactive power.

In phasor form, V=∣V∣∠θvV = |V|\angle\theta_v and I=∣I∣∠θiI = |I|\angle\theta_i. Then

S=VI∗=∣V∣∠θv⋅∣I∣∠−θi=∣V∣∣I∣∠(θv−θi)=∣V∣∣I∣cos⁡ϕ+j∣V∣∣I∣sin⁡ϕ=P+jQ\begin{aligned} S = VI^* &= |V|\angle\theta_v\cdot|I|\angle-\theta_i = |V||I|\angle(\theta_v - \theta_i)\\ &= |V||I|\cos\phi + j|V||I|\sin\phi = P + jQ \end{aligned}

For a load Z=R+jXZ = R + jX: S=∣I∣2Z=∣I∣2R+j∣I∣2XS = |I|^2Z = |I|^2R + j|I|^2X.

Phasor diagram and power triangle

 V reference (lagging load)       Power triangle
  ---------------> V                  /|
  \  phi                         S  /  | Q = |V||I|sin(phi)
    \                             /    |
      \  I (lags V)             / phi  |
        v                      +-------+
                                P = |V||I|cos(phi)

Multiplying V by the conjugate of I turns the V–I phasor diagram into a right-angled triangle. The hypotenuse is ∣S∣|S|, the base is P, the height is Q, and the angle is ϕ\phi.

Significance of the components

ComponentUnitMeaning
P (real part)WAverage power converted to useful work and losses. It is what energy meters record.
Q (imaginary part)varPower exchanged back and forth with magnetic and electric fields. It is needed for magnetising and sets the voltage levels, but does no net work.
∣S∣\lvert S\rvertVASets the current and the rating of generators, transformers and cables
ϕ\phi, cos⁡ϕ\cos\phi—Power factor: the share of S that is useful power
  • Q > 0 means a lagging (inductive) load and Q < 0 a leading (capacitive) load.
  • A low power factor means more current for the same P. This causes more I2RI^2R loss, more voltage drop and larger equipment. So utilities add capacitors to reduce Q.

Example: V=230∠0∘V = 230\angle0^\circ V and I=10∠−36.87∘I = 10\angle-36.87^\circ A give S=2300∠36.87∘=1840+j1380S = 2300\angle36.87^\circ = 1840 + j1380 VA, with pf 0.8 lagging.

✓ Answer checked by Claude Opus 5.5 (high effort)

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