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HELSINKI UNIVERSITY OF TECHNOLOGY Department of Electrical and Communications Engineering Analysis of a 1.7 MVA Doubly Fed Wind-Power Induction Generator during Power Systems Disturbances Slavomir Seman, Sami Kanerva, Antero Arkkio Laboratory of Electromechanics Helsinki University of Technology Jouko Niiranen ABB Oy, Finland Overview • Introduction • The Doubly Fed Induction Generator • Frequency Converter and Control • Crowbar • Modeling of The Network, Transformer and Transmission Line • Simulation Results • Conclusions The Doubly Fed Induction Generator is Rs jks Lrl Lsl j(krr Rr Transient Model of the Generator ir • The machine equations x-y im us Lm ur reference frame fixed with rotor • Constant speed - no equation of movement included P U 1.7 MW N N, stator U (L-L) 690 V (delta) max, rotor n f N N, stator 2472 V (star) 1500 rpm 50 Hz Frequency Converter and Control Model of the Frequency Converter • Two back-to-back connected voltage source inverters (VSI) • DTC • The Network Side Converter - simplification 1-st order filter transfer function • PI controller Udc -level The Rotor Side Converter Model of the Rotor Side Converter • Modified DTC • Input demanded PF or Q , Tref • Voltage vector applied - optimal switching table • The tangential component of the voltage vector controls the torque whereas the radial component increases or decreases the flux magnitude Over-Current Protection - Crowbar Passive Crowbar • over-current protection - the rotor, rotor side converter • no chopper mode • disconnection of the converter rotor is connected to CB U dc U dc max I crow ( ira -ira + irb -irb + irc -irc )/2 • CB is active until MCB disconnects stator from the network U crow Rcrow I crow U CB _ semic Modeling of the Network, Transformer and Transmission Line Modelling of test set-up • Power supply - SG or 3phase V source with short circuit reactance and inductance • Transmission line - R-L equivalent circuit • Transformer - short circuit R-L and stray C, no saturation • Short circuiting TR - R-L equivalent circuit Simulation Results - Voltage Dip without Crowbar Matlab-Simulink, t_step = 0.5e-7, T_ref =0.5 p.u., w_ref = 1.067 p.u., Voltage dip 35% Un 1.5 Stator voltage A - phase Rotor voltage A - phase DC-link voltage vas var udc [p.u.] 1 0.5 0 -0.5 -1 -1.5 4.8 4.9 5 5.1 5.2 5.3 t [s] Voltage dip applied MCB open 5.4 Simulation Results - Voltage Dip without Crowbar 4 Stator current A - phase Rotor current A - phase Electromagnetic torque 3 ias iar Te [p.u.] 2 1 0 -1 -2 4.8 4.9 5 5.1 5.2 5.3 t [s] Voltage dip applied MCB open 5.4 Simulation Results - Voltage Dip with Passive Crowbar Matlab-Simulink, t_step = 0.5e-7, T_ref =0.5 p.u., w_ref = 1.067 p.u., Voltage dip 35% Un 1.5 Stator voltage A - phase Rotor voltage A - phase DC-link voltage vas var udc [p.u.] 1 0.5 0 -0.5 -1 -1.5 4.8 4.9 5 5.1 5.2 5.3 t [s] Voltage dip applied MCB open 5.4 Simulation Results - Voltage Dip with Passive Crowbar 3 Stator current A - phase Rotor current A - phase Electromagnetic torque 2.5 2 ias iar Te [p.u.] 1.5 1 0.5 0 -0.5 -1 -1.5 -2 4.8 4.9 5 5.1 t [s] Voltage dip applied 5.2 5.3 MCB open 5.4 Conclusions • Transient behaviour of DTC controlled DFIG for wind-power applications studied. • The transient simulation results with and without crowbar were compared. • When the crowbar is implemented, the stator and rotor transient current decay rapidly and rotor circuit is properly protected. • Transient electromagnetic torque is reduced by means of crowbar but oscillates longer than in case without crowbar.