Park transform
How it works
The transform is a composition of the Clarke transform and a rotation. Step 1: the three-phase abc quantities are projected onto the stationary αβ frame (Clarke transform), isolating the common-mode (homopolar) part as the zero-sequence component. Step 2: the αβ frame is rotated by the instantaneous electrical angle θ (rotor position) so that the d and q axes spin synchronously with the rotor flux vector. As a result, balanced sinusoidal waveforms at the rotor-speed frequency become constant in the new frame. The inverse Park transform maps the dq quantities back to actual three-phase quantities, e.g. before inverter modulation.
Problem solved
Analyzing and controlling three-phase AC machines is hard because phase quantities vary sinusoidally in time and a synchronous machine's inductances depend on the instantaneous rotor position (a time-varying model). This complicates controller design and torque computation. The Park transform removes that dependence by moving the description into a rotating frame where the quantities become constant and the model becomes linear with constant coefficients.
Components
Component aligned with the rotor flux direction.
Component orthogonal to the d-axis (shifted by 90 electrical degrees).
Homopolar component; zero in a balanced (symmetrical) system.
Instantaneous electrical angle of the rotating reference frame, usually derived from rotor position.
Evolution
Robert H. Park presents the two-reaction theory and the dq0 frame for synchronous machines.
The Park transform becomes the core of FOC for AC motors (Blaschke's work).