International Conference on Renewable Energies and Power Quality (ICREPQ’14) Cordoba (Spain), 8th to 10th April, 2014 Renewable Energy and Power Quality Journal (RE&PQJ) ISSN 2172-038 X, No.12, April 2014 Sliding Mode Control (SMC) of Permanent Magnet Synchronous Generators (PMSG) M.S. Merzoug1, H. Benalla 2 and L. Louze1 1 Department of Electrical Engineering L’arbi Ben M’hidi Oum el bouaghi, University B.P. 358, Oum el Bouaghi 04000 (Algérie) e-mail: [email protected] 2 LEC- Research Laboratory Department of Electrical Engineering Mentouri Constantine,University Abstract. This paper presents Sliding Mode Control of Permanent magnet synchronous generators. A comprehensive dynamical model of the PMSG in d-q frame and its control scheme is presented. Wind energy is a promising technology and becomes more and more interesting player on the market of energy production. Since the converter/capacitor model is nonlinear, the sliding mode technique constitutes a powerful tool to ensure the dc-bus voltage regulation. The simulation results show the method is simple and has high precision of control, and the system has good characteristics in steady state and during transients with permanent magnet synchronous generator. during the last 20 years it has shown to be a very effective control method. Key words For sliding mode controller, Lyaponov stability method is applied to keep the nonlinear system under control SMC provides a fast and accurate dynamic response. Also makes the system response insensitive to changes in parameters and load disturbance. Lyapunov, PMSG, SMC, PWM, IGBT. 1. Introduction Permanent Magnet Synchronous Generators (PMSG) are receiving significant attention from industries for the last two decades. They have numerous advantages over the machines which are conventionally used. Current research in the design of the PMSG indicates that it has high torque to current ratio, large power to weight ratio, high efficiency, high power factor and robustness. Currently, there is much interest in using brushless electronically commutated servo machines in high performance electromechanical systems and the application of neodymium-iron-boron (Nd2Fe14B) and samarium cobalt (Sm1Co5 and Sm2Co17) rare-earth magnets results in high torque and power density, efficiency and controllability, versatility and flexibility, simplicity and ruggedness, reliability and cost, weight-totorque and weight-to-power ratios, better starting capabilities [1]. Sliding mode variable structure control which sliding mode can be designed is insensitive to system parameters change and load disturbance, and has the advantages of good robustness, quick response, and easy realization and so on. Accordingly, hopeful to design a control strategy of high quality by applying sliding mode control (SMC) to the control of PMSM [3]. 2. Mathematical Model Of The PMSM The dynamic model of PMSG has been built in the d-q rotating reference frame, where the q-axis goes ahead 90 from the d-axis with respect to the direction of rotation. The electrical model of the PMSG in the d-q synchronous reference frame, with the voltage and torque equations are given by : [4] [9] d ϕd + ωr ϕq dt d Vq = − R S I q − ϕq − ωr ϕd dt ϕd = L d I d + ϕ ϕq = L q I q Vd = − R S I d − (1) (2) (3) (4) And the electromagnetic torque Te is given by [10]: Sliding mode control (SMC) theory was introduced for the first time the context of the variable structure system (VSS). It has become so popular that now it represents this class of control systems. Even through, in its early stage of development, the SMC theory was over-looked because of the development in the famous linear control theory [2], Te = 3 P[(Ld − Lq )Id Iq + Iq ϕ)] 2 (5) ɺ t) = 0 s(x, (10) u n = − K sgn ( s ) (11) Wher : K > 0 K: is the control gain 1 sgn(s) = 0 −1 Fig. 1.a s>0 s=0 (12 ) s<0 4. The Sliding Mode Application Figure 2, Shows the proposed control scheme in a cascade form in which two surfaces is required Fig. 1.b Fig. 1. Equivalent Circuit of a PMSG in the synchronous reference frame (a) d-axis, (b) q-axis. 3. Description Of Sliding Mode Control The implementation of this control method requires mainly three stages: A. Sliding Surfaces J. Slotine proposes a form of general equation to determine the sliding surface [5]. d s(x, t) = + λ dt n −1 e(t) (6) With: e(t) is the error in the output state e(t) = x ref (t) − x(t) Fig.2. Block diagram of DC Voltage regulation of PMSG using SMC (7) The speed error is defined by: λ is a positive coefficient e = Vdcref − Vdc B. Conditions of convergence The convergence condition is defined by the equation of Lyapunov : S.Sɺ ≺ 0 (8) (13) For n=1, the direct current control manifold equation can be obtained from equation (6) as follow ɺ ɺ ɺ Ω) = V s( dcref − Vdc (14) The best way to calculate the Vdc area is to put it into the following form: C. Controller Design Consequently, the structure of a controller consists of two parts; a first concerning the exact linearization and a second stabilizing. u(t) = u eq (t) + u n A. DC voltage Control [6 8] (9) u eq (t) Corresponds to the equivalent control suggested, It is calculated on basis of the system behaviour along the sliding mode described by: V dV P* = Vdc Idc = Vdc C dc + dc dt R (15) Therefore: 2 dVdc 1 * Vdc = P − dt CVdc R (16) P* = 2 Vdc R Vdn = K d sgn ( s(Id ) ) (17) (30) Where When losses are not taken into electromagnetic torque will be given by: Te = account, the K d : Positive constant C. Quadrature Current Control P* Ω (18) The quadrature current error is defined by: Since: e q = I qref − I q Te = 3 PIq ϕ 2 (19) Then: Iq = 2 P* 3 ωϕ (20) (21) In which: Ieq q Iqn 2 P* = 3 ωr ϕ (22) = K Vdc sgn ( s(Vdc ) ) s(I q ) = I qref − I q (32) ɺ q ) = ɺIqref − ɺIq s(I (33) Vqref = Vqeq + Vqn (34) R L ϕ Vqeq = ɺIqref + s Iq + Pωr d Id + Pωr Lq L L L q q q ( Vqn = K q sgn s(Iq ) ) 5. Converter (24) For n=1, the direct current control manifold equation can be obtained from equation (6) as follow s(Id ) = Idref − Id (25) ɺ d ) = ɺI dref − ɺI d s(I (26) The equivalent circuit of a voltage source converter is presented in Fig.2.2. A sit can be seen in the figure3, a three phase converter has 6 semiconductors (IGBTs) displayed in three legs: a, b and c. The 6 semiconductors are considered as ideal switches. Only one switch on the same leg can be conducting at the same time [8]. Substituting the expression of given by equation (1) in equation (26) we obtain Lq Rs 1 Id − Pωr Iq − Vd Ld Ld Ld (36) Where: K q : Positive constant The direct current error is defined by ɺ d ) = ɺIdref + s(i (35) (23) B. Direct Current Controller [7]: ed = Idref − Id For n=1, the quadrature current control manifold equation can be obtained from equation (6) as follow The control voltage Vqref is defined by: The current control iq is defined by : Vqref = Vqeq + Vqn (31) (27) The control voltage Vdref is defined by: Vdref = Vdeq + Vdn (28) Lq R Vdeq = ɺIdref + s Id − Pωr Iq Ld Ld Ld (29) Fig. 3. Voltage Source Converter In the figure, Sa, Sb, Sc are variables which represent the switching status for each leg. S can only have two values: 1 for the conduction state and 0 for the block state. The desired output voltages are obtained by programming the duty cycles of the 6 IGBTs. High accuracy and strong robustness of the sliding mode control are providing by Fig.6, when resistance load (100 Ω, 10000 Ω) are applied. A rapid response is obtained and the introduced perturbation is immediately rejected by the control system According to for the connection presented in Fig.3 the applied voltages at the machine terminals, Uan, Ubn and Ucn and the DC-link current IDC may be found as 7. Conclusion Uan 2 −1 −1 Sa U DC U bn = 3 −1 2 −1 Sb Ucn −1 −1 2 Sc I DC = Sa Sb i a Sc i b ic (37) In this approach the components I d and I q is regulated (38) C ( (39) ) dVdc 1 V = Sd Vdc + Sq Vdc − dc dt 2 RL using (SMC) control, so that I d is zero, the controller is designed in the total system including switching devices. The simulation results show, Fast response without overshoot and robust performance to parametric variation and disturbances in all the system. And the model of the PWM converter is : 1 Vsd = 2 Sd Vdc V = 1 S V sq 2 q dc A sliding mode control method has been proposed and used for the control of a permanent magnet synchronous generator. Simulation Results show good performances obtained with proposed control, with a good choice of parameters of control. The DC voltage control operates with enough stability. (40) Vdc is the DC voltage 6. Simulation Results Extensive simulations have been performed using Matlab/Simulink software to examine control algorithm of the Sliding Mode Control of permanent magnet synchronous Generator. In order to vali1date the control strategies as discussed, digital simulation studies were made the system described in figure 2. Three phases PMSG parameters: Rs=1.4 Ω, φ=0.154wb, Ld =6.6mH, Lq =5.8mH F=0.00038N.m.s/rad, J=0.00176 kg.m2 The DC voltage regulation is obtained using the proposed algorithm controller in spite of the presence of disturbances such as step changing of the resistive load and the mechanical speed (when the SEIG is driven by a wind turbine for example) The validity of the control is demonstrated through the results shown in Fig. (4, 5, 6) the response for step in DC voltage command is chow in Fig.4, the DC voltage response is completely robust with perfect rejection of load disturbances, Fig.5, show the response of the components id and iq . The stator currents which are controlled by PWM generated by (SMC) control. References [1] N. Selvaganesan1and R. Saraswathy Ramya “A Simple Fuzzy Modeling of Permanent Magnet Synchronous Generator” ELEKTRIKA VOL. 11, NO. 1, 2009, 38-43 Faculty of Electrical Engineering Universiti Teknologi Malaysia. [2] O. Gjinim T. Kaneko and H. Ohaswa. “A new controller for PMSM Servo Drive Based on the Sliding Mode Control with Parameter Adaptation” D 123 N6, 2003 Japan [3] S. Xin, PMSM Servo System Sliding Mode Variable Structure Control, Master's degree thesis, essays of professional control theory and control engineering Wuhan University of Technology, P.R.China 2007 [4] P. Pragasan, and R. Krishnan, “Modeling of permanent magnet motor drives”, IEEE Trans. Industrial electronics, Vol. 35, no.4, Nov. 1988. [5] A. Massoum, M-K. Fellah, A. Meroufe, Sliding mode control for a permanent magnet synchronous machine fed by three levels inverter using a singular perturbation decoupling, Journal Of Electrical & Electronics Engineering. Vol 5. Istanbul university – 2005 [6] L. Louze, A.L. Nemmour, A. Khezzar, M.E. Hacil and M. Boucherma “Cascade sliding mode controller for self-excited induction generator” Revue des Energies Renouvelables Vol. 12 N°4 (2009) 617 – 626 Ohm [7] A. G. Assaoui, M. Abid, “Sensorless Control of Permanent Magnet Synchronous Motors”, 2nd International Conference on Electrical Engineering Design and Technologies November 8-10, 2008 Hammamet, Tunisia [8] M. O. Mora “Sensorless vector control of PMSG for wind turbine applications” Master Thesis, Institute of Energy Technology Aalborg University, June 2009. [9] C. Arroyo, Modeling and simulation of permanent magnet synchronous motor drive system, thesis Master of Science electrical engineering University of Puerto rico Spain, 2006 [10] L. G. González, E. Figueres , G. Garcerá , O. Carranza “Synchronization Techniques Comparison for Sensorless Control applied to PMSG” International Conference on Renewable Energies and Power Quality (ICREPQ’09) Valencia (Spain), 15th to 17th April, 2009 160 250 150 200 D C V o lta g e [V ] S p e e d [ra d /s ] 140 130 120 110 100 150 100 90 50 80 70 0 0.5 1 1.5 2 2.5 0 3 0 0.5 1 1.5 Time [s] 2 2.5 3 2 2.2 Time [s] 2 221 -2 D C V o lta g e [V ] T o rq u e T e [N .m ] 0 -4 -6 -8 220.5 220 219.5 -10 -12 0 0.5 1 1.5 2 2.5 3 219 1 1.2 1.4 Time [s] 1.6 1.8 Time [s] 30 5 20 0 C o u ra n t Id a n d Iq [A ] C o u ra n t Ia [A ] Fig. 4. Response under load disturbance (variation of speed) 10 0 -10 -20 -30 -5 -10 -15 -20 -25 0 0.5 1 1.5 2 2.5 3 -30 Id Iq 0 0.5 1 1.5 Time [s] Time [s] Fig. 5. Stator current under load disturbance 2 2.5 3 250 200 DC Voltage [V] 8000 6000 4000 2000 150 100 50 0 0 0.5 1 1.5 2 2.5 0 3 0 0.5 1 1.5 Time [s] Time [s] 30 20 Courant Ia [A] Resistance RL [Ohm] 10000 10 0 -10 -20 -30 0 0.5 1 1.5 2 2.5 3 Time [s] Fig. 6. Response under load disturbance (Variation of resistive load) 2 2.5 3
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