A Study on Variable Speed Constant Frequency AC Double- Fed Exciting Wind Power Generation System and Its Control Technology

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1165 A publication of CHEMICAL ENGINEERING TRANSACTIONS VOL. 62, 2017 Guest Editors: Fei Song, Haibo Wang, Fang He Copyright 2017, AIDIC Servizi S.r.l. ISBN 978-88-95608-60-0; ISSN 2283-9216 The Italian Association of Chemical Engineering Online at www.aidic.it/cet DOI: 10.3303/CET1762195 A Study on Variable Speed Constant Freuency AC Double- Fed Exciting Wind Power Generation System and Its Control Technology Xuan Zhu, Mao Lin Department of Mechanical Engineering, Hainan University, Hainan 570228, China xuanzhu@163.com As a green and recycling energy, wind energy has attracted more and more attention of the people. Relevant utilization techniues are also becoming more and more deep and mature. Compared with traditional wind power technology, variable speed constant freuency AC double-fed exciting wind power generation technology has more advantages, such as small volume, light weight and high efficiency. For grid-side used in the wind power generation system, a mathematic model under synchronous coordinate system is established and a vector strategy of grid-side based on grid voltage orientation is obtained through detailed derivation accordingly. It mainly describes the grid connection methods of variable speed constant freuency AC double-fed exciting : no-load grid connection, direct grid connection and load carrying grid connection. Based on above theoretical analysis, this paper establishes a set of simulation platform and test bed with rated power 4kW and gives its structure charts. 1. Introduction As is known to all, there are limited fossil energies to be developed and used by human beings on earth, and they are non-renewable. With gradual improvement and speeding of global industrialization process, global countries have a rising demand for energies. But, common coal, petroleum and natural gas are gradually exhausting. In other words, if without ling, fossil energies stored on earth for several hundred million years can be consumed by the human in the following two hundred years (Han et al., 2017). Meanwhile, fossil energies widely used also seriously damage the geoecological environment. For example, carbon dioxide and oxygenated sulphide emitted by burning of fossil fuels can directly cause greenhouse effect and acid rain. Faced with the challenge of sustainable development of society and economy, that how to solve the increasingly urgent energy crisis and relieve the environmental degradation is the major task for social development of human beings (Kim et al., 2017). Currently, global countries have reached an agreement on energy crisis and environmental degradation, i.e. seeking and developing renewable energy sources. On this basis, relevant preferential policies should be prepared to support wide application of new energies. During development and application of multiple renewable energy and new technology, wind energy, one of major members, is paid to many attentions (Liu et al., 2016). This paper mainly studies the variable speed constant freuency AC double-fed exciting wind power generation system. 2. Grid-side model In the variable speed constant freuency AC double-fed exciting wind power generation system, possible running conditions of grid-side and rotor-side are shown in Figure 1 and Figure 2: diagram for running conditions of wind power generation system under secondary-synchronous and supersynchronous speed (Okedu, 2017). When the secondary-synchronous power generation is neglected, the slip s is more than 0; the grid-side is operated in the rectification conditions; rotor-side flows through slip power and is operated in the contravariant conditions; in the super-synchronous power generation conditions, the slip s is less than 0 and rotor-side is operated in the contravariant conditions and only flows through slip power; the grid-side is operated in the feedback status (Wang et al., 2016). Please cite this article as: Xuan Zhu, Mao Lin, 2017, A study on variable speed constant freuency ac double-fed exciting wind power generation system and its technology, Chemical Engineering Transactions, 62, 1165-1170 DOI:10.3303/CET1762195

1166 Power grid (1-s)p Sp (1-s)p Doubly fed transformer RSC GSC Sp Figure 1: Time - to - back power flow Power grid (1- s )p s p (1- s )p Doubly fed transformer RSC GSC s p Figure 2: Super-synchronous power generation power system back - to - back power flow 3. Control strategy of grid-side If the freuency for synchronously rotating d reference coordinate system to same as grid freuency, transfer function of current loop can be directly obtained through the euation and grid-side object model: vd id v i R sl Grid voltage synthesis vector is fixed at d axis of synchronous rotation system, then { v d = const v = 0 It s further simplified according to the object model, i.e. reuirements for vd1 and v1 output by bridge arm should be: * vd1 v 1 vd v ωl ωl i vd i There is current coupling among two voltage loops Ingrid-side model with conversion of d rotary coordinate system, i.e. change of current component i at axis may cause id change through coupling item ωli. Similarly, change of current component id at d axis may cause i change through coupling item ωlid. Such coupling relationship is unbeneficial for design of voltage and current ler. So, grid voltage feedforward compensation and AC-side current cross decoupling are introduced herein (Xu, et al, 2017). (1) (2)

Through simplified block diagram for current inner loop of grid-side after adding grid voltage feedforward and decoupling, it can be seen that the coupling effect is eliminated and vector below ACside current d axis forms two independent loops without mutual influence. They are linear system with single input and single output and independent ler. Below synchronously rotated d reference coordinate, active power and reactive power absorbed by the system from grid side can be expressed as: v i vid P d Q d vi vdi vdid vdi If active power is positive, it means that energy flows from grid to. If reactive power is positive, it means that is inductive to the grid and absorbs the inductively reactive current. It can be seen from circuit structure that if AC-side active power of the is more than active power reuired by the load, excessive power can be used to improve DC capacitor voltage. If AC-side active power is less than active power reuired by the load, the capacitance discharges the energy and the voltage is reduced (Yao Y., 2016). As current component is in direct proportion to active power, the voltage can be led to get the command value of active current component. Generally speaking, grid-side is operated in the rectifier or feedback condition of unit power factor, so command value of reactive current component is set to 0. Voltage loop is led to get reference command of shaft current component, which is directly preset. Then, it s subtracted by actual current component to get the error, which should be input into the ler. Control results, cross decoupling item and grid voltage feedforward compensation are used to get reference voltage need to be input at AC side of the. Through inverse transformation, reference voltage of rotary coordinate system can be changed to a stationary coordinate (Ye, et al, 2016). Voltage in the coordinate can be used to produce drive signals of switch tube of grid-side led by SVPWM. Then, it s necessary to get the system of above grid-side. 4. Direct grid connection, No-load grid connection and Load carrying grid connection As shown in Figure 3, rotor should be firstly disconnected with s, i.e. switch k2 is disconnected and switch k1 is connected. Stator-side of double-fed is directly connected to the grid. At this time, it is euivalent that large inductive load is connected to the grid and main stator current is exciting current with small impact. The DC is started for non-load operation. When its rotating speed is increased to the preset slip range±0.5, it s necessary to connect the switch k2 and start the rotor-side and input exciting power. In this way, the system is directly operated under generation without switching the strategy. As shown in Figure 4, rotor-side is directly connected to the rotor side of double-fed and stator side is connected to the grid through bidirectional thyristor. Control method: DC is adjusted to reach a certain speed, i.e. fixed slip ratio. Before connection of switch k1, i.e. grid connection, rotor-side should be led to achieve that inductive voltage at stator side should have same amplitude, same freuency and same phase as grid-side voltage. Then, bidirectional thyristor k1 is triggered to realize grid connection. 1167 (3) Dual - track K2 Gearbox K1 Network side Figure 3: Variable speed constant freuency AC excitation doubly - fed wind power generation system direct and grid diagram

1168 Dual - track Bidirectional thyristor Gearbox K1 Network side Figure 4: Wind power generation system without load and network diagram As shown in Figure 5, detailed description on disconnection of switch k1 is not described here again. When the system is operated independently with load, the mode has been stated in the chapter 3. When output voltage at stator side of double-fed reaches the grid connection reuirements, it s necessary to give trigger signals to bi-directional non-thyristor switch to trigger connection and grid connection operation. Dual - track load Bidirectional thyristor Gearbox K1 Network side Figure 5: Schematic diagram of wind power generation system with load 5. Characteristics of these grid connection modes During no-load grid connection, voltage at output rotor side modulated by SVPWM after startup of rotor-side includes sub-superior freuency switching harmonics. As stator side is disconnected and not connected with filter capacitor, it means that high-freuency harmonics generated by rotor-side can be transferred from rotor side to stator side. Therefore, in order to get a uality side voltage of stator, filter capacitor should be added to the stator side or between output inductance at rotor side and rotor (filtering high freuency harmonic voltage entering the rotor, inductive voltage at stator side should have no high freuency harmonics). Filter capacitor connected in the stator side, rotor leakage inductance and stator leakage inductance are used to form an output low-pass filter. Filter capacitor connected in the rotor side, output capacitor in the rotor side, rotor leakage capacitor of the and stator leakage capacitor are used to form a LCL filter. Resonant freuency is generally obtained at the place with switch freuency more than 10 times of output voltage freuency and less than one tenth. In addition, filter capacitor connected in the stator side shouldn t be used to excessively compensate for reactive power of the power generator. Otherwise, the system may be excessively excited, especially during non-load, and become instable. Load carrying grid connection and no-load grid connection have same objective and strategy before and after grid connection. The only difference is that current in the stator side is not 0 after loading and current in the stator side should be collected for ling. In extreme conditions, i.e. large load impedance, current in the stator side of the is very small. At this time, there are no obvious different. During actual application, rotor-side and should also provide active power for resistive load. At this time, the power is only determined by the load. Matters to be noticed should be it s prohibited to select too small load.

Because, large power consumed by small load may greatly increase the active power sent by the under rated conditions. 6. Results Motor parameters: Model is Z2-52; rated power is 7. 5kw; rated voltage is 220V; rated current is 41A. Wind power generation system in the simulation and experimental is composed of two subsystems, i.e. gridside subsystem and rotor-side sub- system. Grid-side and rotor-side on the test bed are centered on TMS320LF240. Power device is provided with two units of IGBT modules, which are respectively provided with sampling, PWM pulse generation, display and protection panel. There are no communication device euipment between two s. Independent system can be used for completing their respective functions. Among them, parameters for subsystem of grid-side : AC-side filter inductance is 2.6mH and designed rated current is 14A. Capacitance on the DC bus is 4700μF and bus buffer is RCD. AC-side of gridside is not directly connected to three-phase network, but connected with power grid through threephase transformer with rated capacity 2.5kVA and ratio of transformation 380V/110V. Wiring mode of the transformer is /Y. 1169 DC cabinet Usab Uscb load Ugab Ugbc M Bidirection al thyristor DC θr ira irb inverter Grid side rectifier ia ib SVPWM SVPWM Rotor side VDSP board vector Stator flux vector orientation Grid side vector Grid voltage vector orientation Rectifier side VDSP board Locked phase Locked phase Figure 6: Wind Power Grid - Connected System Simulation and Experimental All simulation results should be obtained through sampling, calculation and ling of the program. As the switch freuency is 5400KHz, i.e. wave data is 1/5400s per point. During simulation, the rotating speed is set to 700r/min. Unless otherwise specified, the horizontal axis should be time axis with unit second in the following simulation results. If it s a voltage diagram, the unit of vertical coordinate should be volt. If current diagram, it should be Ampere. If active power diagram, it should be watt. If reactive power diagram, it should be volt-ampere. System structure of simulation framework platform is shown in Figure 6.

1170 7. Conclusion Through study of variable speed constant freuency AC wind power generation system under independent operation, non-load operation, direct grid connection and load carrying grid connection and other conditions, results show that simulation waveform and test data are basically same as the theoretical analysis, which achieves the expected effects. Reference Han P., Cheng M., Chen Z., 2017, Dual-Electrical-Port Control of Cascaded Doubly-Fed Induction Machine for EV/HEV Applications, IEEE Transactions on Industry Applications, 53, 1390-1398, DOI: 10.1109/TIA.2016.2625770 Kim Y., Kang M., Muljadi E., Park J.W., Kang Y.C., 2017, Power Smoothing of a Variable-Speed Wind Turbine Generator in Association With the Rotor-Speed-Dependent Gain, IEEE Transactions on Sustainable Energy, 8,990-999, DOI: 10.1109/TSTE.2016.2637907 Liu Y., Niu S., Fu W., 2016, Design of an Electrical Continuously Variable Transmission Based Wind Energy Conversion System, IEEE Transactions on Industrial Electronics, 63, 6745-6755, DOI: 10.1109/TIE.2016.2590383 Okedu K.E., 2017, Effect of ECS low-pass filter timing on grid freuency dynamics of a power network considering wind energy penetration, IET Renewable Power Generation, 11, 1194-1199, DOI: 10.1049/ietrpg.2016.0855 Wang Y., Niu S., Fu W.N., Ho S.L., 2016, Design and Optimization of Electric Continuous Variable Transmission System for Wind Power Generation, IEEE Transactions on Magnetics, 52, 1-4, DOI: 10.1109/TMAG.2015.2487995 Xu F., Cheng M., Zhang J., 2017, Multi-objective of direct-driven wind power generation system with freuency separation, Chinese Journal of Electrical Engineering, 3, 42-50, DOI: 10.23919/CJEE.2017.7961321 Yao Y., Cosic A., Sadarangani C., 2016, Power Factor Improvement and Dynamic Performance of an Induction Machine with a Novel Concept of a Converter-Fed Rotor, IEEE Transactions on Energy Conversion, 31, 769-775, DOI: 10.1109/TEC.2015.2505082 Ye H., Pei W., Qi Z., 2016, Analytical Modeling of Inertial and Droop Responses from a Wind Farm for Short- Term Freuency Regulation in Power Systems, IEEE Transactions on Power Systems, 31, 3414-3423, DOI: 10.1109/TPWRS.2015.2490342