Complex Power
In power system analysis the concept of Complex Power is frequently used to calculate the real and reactive power.
This is a very simple and important representation of real and reactive power when voltage and current phasors are known. Complex Power is defined as the product of Voltage phasor and conjugate of current phasor. See Fig-A
Let voltage across a load is represented by phasor V and current through the load is I.
If S is the complex power then,
Let voltage across a load is represented by phasor V and current through the load is I.
If S is the complex power then,
S = V . I*
V is the phasor representation of voltage and I* is the conjugate of current phasor.
So if V is the reference phasor then V can be written as |V| ∠0.
(Usually one phasor is taken reference which makes zero degrees with real axis. It eliminates the necessity of introducing a non zero phase angle for voltage)
(Usually one phasor is taken reference which makes zero degrees with real axis. It eliminates the necessity of introducing a non zero phase angle for voltage)
Let current lags voltage by an angle φ, so I = | I | ∠-φ (current phasor makes -φ degrees with real axis)
I*= | I | ∠φ
So,
S = |V| | I | ∠(0+φ) = |V| | I | ∠φ
(For multiplication of phasors we have considered polar form to facilitate calculation)
Writting the above formula for S in rectangular form we get
S = |V| | I | cos φ + j |V| | I | sin φ
The real part of complex power S is |V| | I | cos φ which
is the real power or average power and the imaginary part |V| | I | sin
φ is the reactive power.
So, S = P + j Q
Where P = |V| | I | cos φ and Q = |V| | I | sin φ
Where P = |V| | I | cos φ and Q = |V| | I | sin φ
It should be noted that S is considered here as a complex number. The real part P is average power which is the average value, where as imaginary part is reactive power which is a maximum value. So I do not want to discuss further and call S as phasor. If you like more trouble I also advise you to read my article about phasor or some other articles on phasor and complex numbers.
Returning to our main point, from the above formula it is sure that P is always more than zero. Q is positive when φ is positive or current lags voltage by φ degrees. This is the case of inductive load. We previously said that inductance and capacitance do not consume power. The power system engineers often say about reactive power consumption and generation. It is said that inductive loads consume reactive power and capacitors produce reactive power. This incorrect terminology creates confusion.
Power Triangle
Returning to the complex power formula, P, Q and S are represented in a power triangle as shown in figure below.
S is the hypotenuse of the triangle, known as Apparent Power. The value of apparent power is |V|| I |
or |S| = |V|| I |
It is measured in VoltAmp or VA.
P is measured in watt and Q is measured in VoltAmp-Reactive or VAR. In power systems instead of these smaller units larger units like Megawatt, MVAR and MVA is used.
The reactive power Q and apparent power S are also important in power system analysis. As just shown above the control of reactive power is important to maintain the voltage within the allowed limits. Apparent power is important for rating the electrical equipment or machines.
or |S| = |V|| I |
It is measured in VoltAmp or VA.
P is measured in watt and Q is measured in VoltAmp-Reactive or VAR. In power systems instead of these smaller units larger units like Megawatt, MVAR and MVA is used.
The ratio of real power and apparent power is the power factor of the load.
power factor = Cos φ = |P| / |S|
= |P| / √(P 2+Q 2)
The reactive power Q and apparent power S are also important in power system analysis. As just shown above the control of reactive power is important to maintain the voltage within the allowed limits. Apparent power is important for rating the electrical equipment or machines.
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