1 Introduction
Wind energy is a renewable energy source with significant development potential. In recent years, wind power technology has garnered extensive attention from scholars worldwide. As a key direction for wind power development, variable-speed constant-frequency (VSCF) technology employs the doubly-fed wind power system as an optimized solution. In this system, the generator’s stator windings connect directly to the grid, while VSCF control is achieved by regulating the frequency, amplitude, phase, and phase sequence of the rotor winding power supply. Since the converter only transmits slip power, its capacity can be significantly reduced.
Currently, doubly-fed wind power systems primarily use AC/AC or AC/DC/AC converters. AC/AC converters have been largely replaced by voltage-source AC/DC/AC converters due to their high output harmonics, low input power factor, and excessive power devices. Although matrix converters have been explored for doubly-fed systems, their complex structure, high voltage endurance requirements, and non-decoupled input/output control limit their adoption in wind power applications.
This study develops a voltage-source AC/DC/AC doubly-fed wind power system controlled by dual DSPs. The grid-side converter adopts voltage-oriented vector control, and the rotor-side converter uses stator-flux-oriented vector control. Experiments confirm that the system supports bidirectional power flow, independent input/output power factor regulation, low harmonic distortion, stable wide-range operation, and high-quality power generation from unstable energy sources like wind.
2 System Configuration
As shown in Figure 1, the system comprises five parts:
Key Details
3 Vector Control for Doubly-Fed Generator
3.1 Control Principles
In the synchronous rotating frame (d-axis aligned with stator flux), the doubly-fed generator model is:
usd=Rsisd+dψsddt−ωsψsq{u_{sd} = R_s i_{sd} + \frac{d\psi_{sd}}{dt} - \omega_s \psi_{sq}}usd=Rsisd+dtdψsd−ωsψsq
usq=Rsisq+dψsqdt+ωsψsd{u_{sq} = R_s i_{sq} + \frac{d\psi_{sq}}{dt} + \omega_s \psi_{sd}}usq=Rsisq+dtdψsq+ωsψsd
urd=Rrird+dψrddt−ωslipψrq{u_{rd} = R_r i_{rd} + \frac{d\psi_{rd}}{dt} - \omega_{\text{slip}} \psi_{rq}}urd=Rrird+dtdψrd−ωslipψrq
urq=Rrirq+dψrqdt+ωslipψrd{u_{rq} = R_r i_{rq} + \frac{d\psi_{rq}}{dt} + \omega_{\text{slip}} \psi_{rd}}urq=Rrirq+dtdψrq+ωslipψrd
Flux equations:
ψsd=Lmims+Lsisd=Lmims{\psi_{sd} = L_m i_{ms} + L_s i_{sd} = L_m i_{ms}}ψsd=Lmims+Lsisd=Lmims
ψsq=−Lmirq{\psi_{sq} = -L_m i_{rq}}ψsq=−Lmirq
ψrd=Lrird+Lmisd{\psi_{rd} = L_r i_{rd} + L_m i_{sd}}ψrd=Lrird+Lmisd
ψrq=Lrirq+Lmisq{\psi_{rq} = L_r i_{rq} + L_m i_{sq}}ψrq=Lrirq+Lmisq
Torque equation:
Te=−npLmimsirqLs{T_e = -\frac{n_p L_m i_{ms} i_{rq}}{L_s}}Te=−LsnpLmimsirq
Neglecting stator resistance voltage drop, stator flux satisfies:
ψsd≈usq/ωs,ψsq≈0{\psi_{sd} \approx u_{sq}/\omega_s, \quad \psi_{sq} \approx 0}ψsd≈usq/ωs,ψsq≈0
Control strategy:
3.2 Grid Control
4 Grid-Side Rectifier Vector Control
In the two-phase synchronous rotating frame (d-axis aligned with phase-A voltage), the PWM rectifier model is:
ud=Ldiddt+Rid−ωsLiq+sdudc{u_d = L\frac{di_d}{dt} + R i_d - \omega_s L i_q + s_d u_{dc}}ud=Ldtdid+Rid−ωsLiq+sdudc
uq=Ldiqdt+Riq+ωsLid+squdc{u_q = L\frac{di_q}{dt} + R i_q + \omega_s L i_d + s_q u_{dc}}uq=Ldtdiq+Riq+ωsLid+squdc
Cdudcdt=32(sdid+sqiq)−iload{C\frac{du_{dc}}{dt} = \frac{3}{2}(s_d i_d + s_q i_q) - i_{\text{load}}}Cdtdudc=23(sdid+sqiq)−iload
Power equations:
P=udid,Q=udiq{P = u_d i_d, \quad Q = u_d i_q}P=udid,Q=udiq
Control logic:
5 Experimental Results
Key Verifications:
6 Conclusion
This study develops a dual-DSP-based voltage-source AC/DC/AC doubly-fed wind power system. Combined with grid-side voltage-oriented and rotor-side stator-flux-oriented vector control, experiments demonstrate: