System Controlling: Dynamic model of a PMSM
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Monday, October 29, 2012

Dynamic model of a PMSM

The two phase equivalent circuit is widely used to analyse the permanent magnet synchronous machine. In this blog I will present the two phase equivalent circuit of the PMSM dynamic model. 
The three phase electrical dynamic equations can be written as:
USa=RsISa+dψSadtUSb=RsISb+dψSbdtUSc=RsISc+dψScdt

where the index $S$ denotes the stator coordinate system.
Also the motor model can be express in the rotating coordinate system
UR=RsIR+dψRdt+jωψR

Now we can write in the two phase equivalent circuit which is rotating with the same frequency as the rotate magnetic field.
ud=RsId+dψddtωψq

uq=RsIq+dψqdt+ωψd

where
ψd=LdId+Lm

ψq=LqIq

The produced torque can be expressed as:
Te=3P2(LmIq+(LdLq)Id)Iq

and the motor dynamics can be represented by:
Te=Jdωrdt+Bωr+TL
 

Coordinate transformation 

Figure 1. PMSM
As you can see in figure 1, the three phase stationary reference frame can be transformed directly into a two phase reference frame using Park's transformation. Let X represent any of the variables (current, voltage, fluxe), the transformation matrix is given by[4]
[XdXqX0]=23[sin(θ)sin(θ2π3)sin(θ+2π3)cos(θ)cos(θ2π3)cos(θ+2π3)121212][XaXbXc]
The transformation can be a combination of two transformations. First the three phase reference frame can be transformed into a two phase reference frame($abc$ to $\alpha\beta$) by replacing $\theta$ with 0
[XαXβX0]=23[0323211212121212][XaXbXc]
The second transformation is a conversion from stationary to rotating reference frame ($\alpha\beta$ to $dq$)
[XdXqX0]=[cos(θ)sin(θ)0sin(θ)cos(θ)0001][XαXβX0]

Appendix:

$P$ - Pole pairs
$R$ - Stator phase resistance
$L_m$ - Permanent magnets flux
$B$ - Viscous friction coefficient
$J$ - Inertia
$L_d$ - Direct axis inductance
$L_q$ - Quadrature axis inductance
$\omega$ - Angular velocity

Sources:

  1. Dal Y. Ohm: DYNAMIC MODEL OF PM SYNCHRONOUS MOTORS
  2. Wikipedia: dqo transformation
  3. Mohamed S. Zaky: Adaptive and robust speed control of interior permanent magnet synchronous motor drives
  4. Lecture Set 6.pdf

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