Let a three-phase system (voltages, currents, flux linkages) be represented by a single complex time-varying vector in a stationary two-dimensional plane (the $\alpha\beta$-plane). For a set of phase quantities $x_a, x_b, x_c$ satisfying $x_a + x_b + x_c = 0$, the space vector is defined as:
where $a = e^{j2\pi/3}$. The factor $2/3$ ensures that the magnitude of $\vec{x}_s$ equals the peak amplitude of a balanced sinusoidal phase quantity. Let a three-phase system (voltages, currents, flux linkages)
For over a century, the analysis of electrical machines has been dominated by the equivalent circuit and the per-phase phasor diagram. This approach, born from the convenience of single-phase power systems, treats a three-phase machine as three independent, magnetically coupled circuits. It works—but only just. It obscures the fundamental gestalt of the rotating field. It requires artificial constructs (mutual leakage, d/q transformations with ad hoc alignments) and fails to reveal the deep topological unity between a squirrel-cage induction motor, a synchronous reluctance machine, and a permanent magnet servo drive. For over a century, the analysis of electrical
$$\vec{v}_s = R_s \vec{i}_s + \frac{d\vec{\psi}_s}{dt} + j \omega_k \vec{\psi}_s$$ It obscures the fundamental gestalt of the rotating field