Three phase phasor proof or simplification

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SUMMARY

The forum discussion centers on the mathematical proof and simplification of three-phase phasors and space vectors, specifically the expression for current in a three-phase system: i(t) = I(cos(wt)<0 + cos(wt - 120)<120 + cos(wt - 240)<240) = 3/2 * I < wt. Participants clarify that phasors and space vectors are distinct concepts; phasors are time-invariant representations of sinusoidal functions, while space vectors map real-valued functions to complex values. The conversation emphasizes the importance of converting terms to their complex representation for simplification and understanding.

PREREQUISITES
  • Understanding of phasors and their time-invariant properties.
  • Familiarity with space vector transformations in electrical engineering.
  • Knowledge of trigonometric identities and complex numbers.
  • Basic algebraic manipulation skills for complex expressions.
NEXT STEPS
  • Study the derivation of the space vector transformation in three-phase systems.
  • Learn about the application of trigonometric identities in simplifying complex expressions.
  • Explore the differences between phasors and complex numbers in electrical engineering contexts.
  • Investigate the implications of using space vectors in dynamic versus steady-state analysis.
USEFUL FOR

Electrical engineers, students studying power systems, and anyone interested in the mathematical foundations of three-phase electrical systems will benefit from this discussion.

  • #31
milesyoung said:
Say you have some complex number ##z = re^{j\phi}##. The ##re^{j\phi}## bit is its polar form, which you can think of as a vector in the complex plane with magnitude ##r## and angle (phase) ##\phi##.

The complex number ##\frac{3}{2}e^{j\omega t}## then represents a vector of constant magnitude ##\frac{3}{2}##, which is rotating counterclockwise in the complex plane with angular frequency ##\omega##. See here for an illustration.

That's exactly the result you would expect in the framework of space vectors as they relate to electrical machines.

The vector shows you what happens if you apply a balanced set of three-phase currents to the stator of a symmetrical machine: it produces a stator current space vector, which rotates CCW in the plane normal to the rotor axis of the machine. There's no actual current with any spatial direction, that's nonsense, but the stator current space vector is aligned with the magnetic axis of the resulting stator field, which makes it a very useful abstraction (and one of the many great properties of space vectors).
Hey I'm back, sorry about the delay.
Ok this is really dumb question but:
I see how the phasee shifted cos-es are adding up to 3/2 with the frequency omega. But the way w're representing it with e^jwt
with the circle on the left hand side, does that imply that the y-axis is actually the imaginary axis?
Cheers
 
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  • #32
tim9000 said:
I see how the phasee shifted cos-es are adding up to 3/2 with the frequency omega. But the way w're representing it with e^jwt
with the circle on the left hand side, does that imply that the y-axis is actually the imaginary axis?
Yes, did you have a look at the Wikipedia page?
 
  • #33
milesyoung said:
Yes, did you have a look at the Wikipedia page?
I did, it's what I based my assertion. It just seems odd to me that we would model this circular path that takes place in an imaginary and real set of axies, to represent the actual vector of the peak mmf in real life. I can accept it though.
 
  • #34
tim9000 said:
It just seems odd to me that we would model this circular path that takes place in an imaginary and real set of axies, to represent the actual vector of the peak mmf in real life.
There's nothing in the framework of space vectors that you can't also express with vectors and matrix algebra, see, for example, the equivalent Alpha–beta transformation, but the algebra of complex numbers is often preferred by electrical engineers. You can just think of the real and imaginary components as coordinates in a plane (the complex plane).
 

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