International Journal for Research and Development in Engineering (IJRDE) www.ijrde.com ISSN: 2279-0500 Special Issue: pp- 270-277 Design of Wind Driven PMSG Based Z-Source Inverter fed Three Phase load for Stand-Alone Applications G.Arthiraja1, M. Ammal Dhanalakshmi2, Dr. M. Sasikumar3 1,2 PG Scholar, 3Professor,Head of the Department EEE Jeppiaar Engineering College, Chennai. Abstract—This paper presents the development of design, modeling and simulation for variable speed wind turbine coupled PMSG based ZSI are simulated through computer software tool using MATLAB/SIMULINK. A variable wind speed turbine coupled Permanent Magnet Synchronous Generator with power electronics interface is modeled for dynamic simulation analysis. The MATLAB/SIMULINK is provided to implements the wind driven PMSG based ZSI for stand-alone application components models and equations. Controllable Impedance source inverter strategies are intended for capturing the maximum power under variable speed operation and maintaining reactive power generation at a pre-determined level for constant power factor control or voltage regulation control. Control schemes for both wind turbine and Permanent Magnet Synchronous Generator are constructed by user-define function provided in the simulation. Simulation case studies provide the variable speed wind Permanent Magnet Synchronous Generator dynamic performance for changes in different wind speed. This control scheme of this model can be employed to regulate the real power, reactive power, generated voltage and generated speed at different wind speed in the power system. Simulation results of this model can be validate the real power, reactive power, generated voltage and generated speed at different wind speeds in the power system. Its simulations results are presented. Index Terms—Wind turbine, variable speed, Permanent Magnet Synchronous Generator, Impedance source inverter, Power electronics interface, Reactive power control. generators including speed control. Many works have been proposed for studying the behavior of PMSG based wind turbine system connected to the load. Most existing models widely use PWM technique for three phase PWM inverter and the output of the inverter is fed to load here Induction motor is acting as a load. Wind electrical power system are recently getting lot of attention, because they are cost competitive, environmental clean and safe renewable power sources, as compared fossil fuel and nuclear power generation capability of design, modeling, simulating and analyzing the dynamic performance of a variable speed wind energy conversion system using MATLAB/SIMULINK. The modeled system includes a fixed-pitch type wind blades, a direct-drive Permanent Magnet Synchronous Generator without a gear-box, and a controllable power electronics system, which consists of a six-diode rectifier and three phase inverter. The entire schematic diagram of the modeled wind generation is shown in Fig. 1. Models of the elements and the system control scheme are proposed in the form of mathematical equations and graphical control blocks and implemented in MATLAB/SIMULINK [2]. The simulation results demonstrate the modeling work provide a reliable and useful simulation tool for evaluating the dynamic performance of a variable speed wind turbine integrated into power system. I. INTRODUCTION Wind energy generation equipment is most often installed in remote, rural areas. Wind energy has been the subject of much recent research and development. In order to maximize the wind energy capture, many new wind farms will employ variable speed wind turbine. PMSG (Permanent Magnet Synchronous Generator) is one of the components of Variable speed wind turbine system. PMSG offers several advantages when compared with fixed speed Fig. 1 Schematic representation of modeled VSWT coupled Permanent Magnet Permanent Magnet Synchronous Generator. Methods Enriching Power and Energy Development (MEPED) 2014 270 | P a g e International Journal for Research and Development in Engineering (IJRDE) www.ijrde.com ISSN: 2279-0500 Special Issue: pp- 270-277 II. MATLAB/SIMULINK BASED MODELING (2) The variable speed wind turbine model consists of the following components. - Wind model - Wind turbine and control - Permanent Magnet Synchronous Generator - Rectifier and inverter (3) (4) Where λ = tip speed ratio M = blade angular speed [mechanical rad/s] R = blade radius [m] VWIND = wind speed [m/s] PM = mechanical power from wind blades [kW] l = air density [kg/m3] CP = power coefficient TM = mechanical torque from wind blades [N-m] Fig. 2 Components of a VSWT coupled Permanent Magnet Synchronous Generator MATLAB/SIMULINK simulation model. Fig.2 depicts the component blocks Components of a VSWT coupled Permanent Magnet Synchronous Generator Matlab/Simulink simulation model. For modeling the shaft and Permanent Magnet Synchronous Generator, models provided by the Matlab/Simulink are used, and models of the wind speed, the wind turbine, power electronics block and the control block are built into the Matlab/Simulink. The mechanical torque obtained from equation (4) enters into the input torque to the Permanent Magnet Synchronous Generator, and is driving the generator. CP may be expressed as a function of the tip speed ratio (TSR) λ given by equation (2) [5]. (5) Where A. Wind Model A wind model selected for this study is a fourcomponent Mode l [3], and can be described by equation (1). VWIND = VBASE + VGUST + VRAMP + VNOISE (1) Where, VBASE = base wind speed [m/s] VGUST = gust wind component [m/s] VRAMP = ramp wind component [m/s] VNOISE = noise wind component [m/s] The base component is a constant speed and wind gust component can be usually expressed as a sine or cosine wave function [4]. In this simulation, wind speed can be representing the constant block in Matlab/Simulink. B. Wind Turbine The wind turbine is described by the following equation (2), (3) and (4) β is the blade pitch angle. For a fixed pitch type the value of β is set to a constant value. C. Permanent Magnet Synchronous Generator The Matlab/Simulink provides a fully developed synchronous Permanent Magnet Synchronous Generator model, which is based on generalized machine theory [2] and with this model both subtransient and transient behavior can be examined. It is considered that the Permanent Magnet Synchronous Generator is equipped with an exciter identical to IEEE type 1 model [6]. The exciter plays a role of meeting the dc link voltage requirement. Since the Permanent Magnet Synchronous Generator is a direct drive type with low speed and a high number of poles, the wind turbine and the generator are rotating at the same mechanical speed via the same shaft. Therefore, shaft dynamics can be characterized by a swing equation on a single mass rotating shown in equation (6). The shaft Methods Enriching Power and Energy Development (MEPED) 2014 271 | P a g e International Journal for Research and Development in Engineering (IJRDE) www.ijrde.com ISSN: 2279-0500 Special Issue: pp- 270-277 dynamics and the rotating mass can be represented by multi-mass torsional shaft model of Matlab/Simulink, which can be easily interfaced with the synchronous machine model Impedance source inverter it convert into ac and inverter output is given to voltage load system. (6) Where JM = a single rotating inertia [kg-m2] TE = electric torque produced by generator [N-m] D = damping [J-s/rad] In variable speed operation, the rotating speed of the wind generator is not consistent with the electrical synchronous speed of the electric network and generally much slower than the speed. The electrical base frequency of the machine in the built-in models must be set to a value corresponding to the rated mechanical speed of the wind turbine specified by a manufacturer or a designer. Equation (7) and (8) give the value for the electrical base speed of the synchronous machine wB.. (7) (8) Where fB = electrical base frequency of the generator [Hz] P = number of poles RPMTUR = mechanical rated speed of the turbine [rpm] Fig. 3 Rectifier and inverter model. The ZSI is a voltage harmonic source in the point view of ac system and a harmonic filter need be placed appropriately to reduce the voltage harmonics it generates [8]. A L-C harmonic filter consisting of a series interconnection inductor and a parallel capacitor is located at the ZSI terminal. Fig. 4 shows a rectifier and ZSI system model that has been implemented in Matlab/Simulink. The six diodes rectifier converts ac power generated by the wind generator into dc power in an uncontrollable way and so control has to be implemented by the power electronics inverter. Current-controlled ZSIs can generate an ac current which follows a desired reference waveform so can transfer the captured real power along with controllable reactive power. For the modeling study, DQ control method that is widely used for ZSI current control is employed. Variables in the ABC three phase coordinates may be transformed into those in the d-q reference frame rotating at synchronous speed by the rotational d-q transformation matrix [2]. In the threephase balanced system, the instantaneous active and reactive power outputs, P and Q, of the wind turbine are described by equation (9). D. Power Electronics Control Several types of power electronics interfaces have been investigated [7]. In this study, system is interfaced with a six diode rectifier and three phase Impedance source inverter which is less expensive than others and commonly put into industrial use, has been modeled for AC-DC–AC conversion. . Fig. 3 shows a rectifier model and inverter model. The six diodes rectifier converts ac power generated by the wind generator into dc power in an uncontrollable way and it is given to (9) Where VD = d-axis voltage at the wind turbine VQ = q-axis voltage at the wind turbine ID = d-axis current at the wind turbine IQ = q-axis current at the wind turbine. Here, VQ is identical to the magnitude of the instantaneous voltage at the wind generation system Methods Enriching Power and Energy Development (MEPED) 2014 272 | P a g e International Journal for Research and Development in Engineering (IJRDE) www.ijrde.com ISSN: 2279-0500 Special Issue: pp- 270-277 and VD is zero in the rotating d-q coordinates, so the equation (9) may be contracted into simpler equation (10). (10) where |VO| is the instantaneous voltage magnitude of the wind turbine system. Since the voltage remains at a level of the load AC voltage and the voltage variation is very small compared to changes in the magnitude of IQ and ID, P and Q are mainly subject to the d-axis current and q-axis current respectively. Fig. 4 illustrates DQ control decouples real and reactive components and enables real power and reactive power to be separately controlled by specifying the respective reference values of PREF and QREF for the both power outputs and independently adjusting the magnitude of the d-axis current IQ and that of the q-axis current ID. The reference values PREF and QREF of the wind generation are specified by what ZSI’s control strategies are taken for real and reactive power output. The firing signals are generated by the sine pulse width modulation (SPWM) technique. The desired current vector IABC_REF and the actual output current vector IABC_WT of the wind system are compared and The maximum aerodynamic power available from wind energy can be described by equation (11) . This simply means that the maximum power may be achieved by varying the turbine speed with varying wind speed such that at all times it is on the track of the maximum power curve [1], [9]. One way of enabling the maximum power capture is to specify the reference value of real power for the inverter control as the available maximum power multiplied by the inverter efficiency, as shown in equation (12). (11) (12) Where CP MAX= the maximum power coefficient λ OPT = value of λ where CP MAX= CP ( λ OPT) η = electrical loss in generator and inverter F. Reactive Power Control Various control modes can be used for determining the amount of reactive compensation to provide. Possible control modes include power factor, Kvar, current and voltage. Constant power factor mode and voltage regulation mode are implemented in this analysis. In constant power factor control (PFC) mode, the reference value of the reactive power of the wind turbine, QREF, may be specified by equation (13). (13) Where PF is power factor and PREF is the reference value of real power output of the VSWT. Fig. 4 Current control scheme of a Impedance source inverter The error signal vector IERR is compared with a triangle waveform vector to create the switching signals. E. Capturing the maximum power In voltage regulation (VR) mode, reactive power compensation is controlled in such a manner that the voltage magnitude of the VSWT-connected bus being kept constant at a specified level. The reference magnitude of the voltage to be regulated must be set as the nominal voltage of the AC load where the wind turbine is considered as being interconnected. Whether the mode controls constant power factor or voltage, the reactive power capability of a VSWT is limited. Such a limitation is required to be considered in the modeling Methods Enriching Power and Energy Development (MEPED) 2014 273 | P a g e International Journal for Research and Development in Engineering (IJRDE) www.ijrde.com ISSN: 2279-0500 Special Issue: pp- 270-277 study. The reactive capability limits of the wind turbine used in this study are determined by MVA rating of the inverter which may be described by equation (14). Continuous powergui signalrms (14) Where QLIMITS, PINV and SINV are the reactive power limits, thereal power output and MVA rating of the inverter respectively. RMS signalrms RMS 5 Display 8 Scope 6 + v - M4 Scope 2 g D P6 M3 S Subsystem Conn1 P4 S M1 g D g D P2 Volt1 S L2 III. MATLAB/SIMULINK STUDIES OF PROPOSED SYSTEM Display Tm c1 A c2 m B + v - Conn2 C Asynchronous Machine SI Units Out1 p5 M7 Scope 11 Gain P3 g D g D P5 S L1 -K- <Rotor speed (wm)> <Electromagnetic torque Te (N*m)> g D M5 Scope 10 S S M6 Fig.6.Simulink Model of PMSG based Three phase ZSI fed Induction motor load. Fig. 5 Matlab/Simulink model of VSWT coupled Permanent Magnet Synchronous Generator interfaced with power electronics The proposed model is implemented into Matlab/Simulink computer software tool and simulated for analyzing the dynamic behaviors of a wind turbine with varying wind conditions. Fig. 5 shows a VSWT based PMSG model implemented in Matlab/Simulink. It indicates wind turbine model, Permanent Magnet Synchronous Generator model, power electronics model with power load system and control blocks. The generated voltage of the Permanent Magnet Synchronous Generator is step up the voltage using step up transformer (0.6kv/2.5k). The step up voltage is given to the power electronics interface of the load system which consists of rectifier and inverter. The inverter output is again step up to 130kv using step up transformer. The detailed explanation of each component of the proposed system was already discussed in section II. The above simulink model describes that the generated voltage is fed with the impedance source network and the inverter output voltage is given to the three phase induction motor. Here the impedance source inverter does both buck and boost operation. The inductor and capacitances design is chosen depend upon the application. The induction motor rotor speed and torque is observed. IV. SIMULATION RESULTS ANALYSIS OF VSWT BASED PMSG. The rating capacity is chosen to be 1.5 MVA and real power 1.5 MW. The rated speed of the rotor is chosen to be 40 rpm. The rated wind speed is 8 m/s. the cut-in and cut-out speeds are 4 m/s and 16 m/s respectively. The switching frequency of the load interface inverter is 1.040 kHz. The capacitor value of load interface rectifier is 2500uF and d.c link voltage is 2.5 kv. The generated voltage of Permanent Magnet Synchronous Generator is 0.6kv. The transformer rating of load connected side is 2.5k/130kv. The p.u voltage magnitude of primary of the transformer is 0.99 p.u. The maximum value of Cp is 1.2. the proposed system operate the unity power factor control. Methods Enriching Power and Energy Development (MEPED) 2014 274 | P a g e International Journal for Research and Development in Engineering (IJRDE) www.ijrde.com ISSN: 2279-0500 Special Issue: pp- 270-277 Fig.10.Simulation results of VSWT based PMSG generated speed. Fig.7.Simulation results of VSWT based PMSG generator voltage. V. SIMULATION RESULTS ANALYSIS OF ZSI FED INDUCTION MOTOR LOAD The Impedance source inverters (ZSI) are used to regulate the speed of three-phase squirrel cage motors by changes the frequency and the voltage and consist of input rectifier, DC link and output converter. They are available for low voltage range and medium voltage range. The value of inductance L1 and L2 is chosen depend upon the application. In this project the value is chosen for inductor is L1 = L2 = 2MH and the value for capacitor C1 = C2 = 2200µf. the operating frequency is 10Khz. The parameters of three phase induction motor load are 5HP horse power, voltage is 420V, current is 8Amps, frequency is 60Hz and rotor type is squirrel cage. Fig.8. Simulation results of VSWT based PMSG generated three phase current Fig.11. simulation results of three phase ZSI output Voltage. The fig.11. shows the three phase ZSI output voltage of the three phase impedance source inverter fed induction motor. The output voltage value is 380V AC Fig.9. Simulation results of VSWT based PMSG generated three (peak voltage). The fig.12. shows the simulation results phase voltage. Methods Enriching Power and Energy Development (MEPED) 2014 275 | P a g e International Journal for Research and Development in Engineering (IJRDE) www.ijrde.com ISSN: 2279-0500 Special Issue: pp- 270-277 of speed of Induction motor. The rotating speed of induction motor is 1500RPM which is achieved by the output voltage of an impedance source inverter. The fig.13. shows the simulation results of generated torque of an Induction motor. The generated electromagnetic torque for three phase impedance source inverter fed induction motor achieved is 40 Tm. The fig.14. shows the simulation results of switching pulses of ZSI. The value of pulse amplitude is 1V and the value of pulse width is 33.3% of period, and the time period is 0.02 sec. Fig.14. simulation results of switching pulses of ZSI. VI. CONCLUSIONS Fig.12.simulation results of speed of Induction motor. Fig.13. simulation results of generated torque of an Induction motor. A dynamic model of a variable speed wind generation with power electronic interface was proposed for computer software tool simulation study and implemented in Matlab/Simulink. Component models of a VSWT and its control scheme have been built by using matlab function block and control block provided in the software. A wind model was integrated into the modeling to see the wind impact. Dynamic responses of the wind turbine to varying wind speeds and under different reactive control schemes were simulated and analyzed based on the modeled system. In the view point of electric utilities, load interface of intermittent generation sources such as wind turbines has been a challenge that can cause lower power quality in power systems. So comprehensive impact studies are absolutely necessary before wind turbines being added to real networks. Also, users who intend to install wind turbines in networks must ensure their systems meet the requirements for load connection. Therefore, the work done in this study provides a reliable tool for evaluating the performance of variable speed wind turbines and their impacts on power networks in terms of dynamic behaviors as a preliminary analysis for their actual integrations and operations. VII. REFERNCES [1] Seyed Mohammad Dehghan,MustafaMohamadian, and AliYazdianVarjani, “ A new variable speed wind energy conversion system Using permanent magnet synchoronus generator and Z-source inverter”. IEEE transactions on energy conversion, vol.24,no.3. September 2009. Methods Enriching Power and Energy Development (MEPED) 2014 276 | P a g e International Journal for Research and Development in Engineering (IJRDE) www.ijrde.com ISSN: 2279-0500 Special Issue: pp- 270-277 [2] E. Spooner and A. C. Williamson, “Direct coupled permanent magnet generators for wind turbine applications,” Inst. Elect. Eng. Proc., Elect. Power Appl., vol. 143, no. 1, pp. 18,1996. [3] N. Yamamura, M. Ishida, and T. Hori, “A simple wind power generating system with permanent magnet type synchronous generator,” in Proc.IEEE Int. Conf. Power Electron. Drive Syst., 1999, vol. 2, pp. 849–854. [4] S. H. Song, S. Kang, and N. K. Hahm, “Implementation and control of grid connected AC– DC–AC power converter for variable speed wind energy conversion system,” Appl. Power Electron. Conf. Expo., vol. 1, pp. 154–158, 2003. [5] A. M. Knight and G. E. Peters, “Simple wind energy controller for an expanded operating range,” IEEE Trans. Energy Convers., vol. 20, no. 2, pp. 459– 466, Jun. 2005. [6] T. Tafticht, et al, “Output power maximization of a permanent magnet synchronous generator based standalone wind turbine,” in Proc. IEEE ISIE 2006, Montreal, QC, Canada, pp. 2412–2416. [7]M. Chinchilla, S. Arnaltes, and J. C. Burgos, “Control of permanent magnet generators applied to variable-speed wind-energy systems connected to the grid,” IEEE Trans. Energy Convers., vol. 21, no. 1, pp. 130–135, Mar. 2006. [8]F. Z. Peng, “Z-source inverter,” IEEE Trans. Ind. Appl., vol. 39, no. 2,pp. 504–510, Mar./Apr. 2003. [9]F. Z. Peng, M. Shen, and Z. Qian, “Maximum boost control of the Z-source inverter,” IEEE Trans. Power Electron., vol. 20, no. 4, pp. 833–838, Jul. 2005. [10]F. Z. Peng, A. Joseph, J.Wang, andM. Shen, “Zsource inverter for motor drives,” IEEE Trans. Power Electron., vol. 20, no. 4, pp. 857–863, Jul. 2005. [11]P. C. Loh, D. M. Vilathgamuwa, C. J. Gajanayake, Y. R. Lim, and C. W. Teo, “Transient modeling and analysis of pulse-width modulated Z-source inverter,” IEEE Trans. Power Electron., vol. 22, no. 2, pp. 498– 507, Mar. 2007. Methods Enriching Power and Energy Development (MEPED) 2014 277 | P a g e