Comparative Analysis in Properties of all Types of Z-Source Inverters (Full text in English) Hongsheng SU1, Hongjian LIN1 1 School of Automation & Electrical Engineering, Lanzhou Jiaotong University, China Abstract The traditional Z-source inverter and its other improved topologies are proposed in this paper. With boost and buck capacity, traditional Z-source inverter has advantages of current and voltage inverters that both the current source and the voltage source inverters can be connected with its DC bus and then inductive and capactive loads can be used as its AC loads. In addition, the dead time is unnecessarily added to prevent upper and lower switching devices of each phase leg in three-phase inverter bridge from conducting simultaneously. Aiming at the shortcomings of the traditional Z-source inverter, two kinds of improved Z –source inverters, quasi Z-source inverters and other enhanced Z-source inverters are analysed in this paper. They overcome the shortcomings of traditional Z-source inverter, but they achieve the boost by inserting shoot-through zero vectors into traditional zero vectors, this will reduce quality of AC output voltage in SVPWM. Finally, two kinds of isolated shoot-through Z source inverters are introduced in this paper, they utilize controlled devices to achieve the separation between shoot-through zero vectors and traditional zero vectors ,so that they make sure higher quality of output voltage. Based on the comparative analysis on each Z-source inverter, using MATLAB to verify the correctness of theoretical analysis in the end. Keywords: Z-source inverters, traditional zero vector, shoot-through zero vector, comparative analysis, simulation 1. Introduction Conventional inverter has either voltage source inverter or current source inverter. The former has buck property, its AC side load is an inductive load. The latter has boost property; its AC side load is a capacitive load [1]. For output voltage of the inverter AC side being lower than the DC voltage and a wide range variation of input voltage, DC / DC chopper circuit often needs to be added, which increases the complexity of the control system and reduces the efficiency of the system. What’s more, in order to prevent the upper and lower devices of each phase leg break-over at the same time and thus damage the devices, the dead time should be added to the switching signal of devices, but this results in the waveform distortion of AC output voltage instead [2]. To overcome the shortcomings of the inverter mentioned above, Professor Peng Fangzheng proposed Z-source inverter in 2003[3]. The inverter make the shootthrough phenomenon of the upper and lower devices of each phase leg become a normal state by using its unique impedance networks while conducting its work [4] and also avoids the distortion of output voltage waveform because of insertion of the dead time insertion as well as simplify the circuit[5]. However, traditional Z-source inverter also remains many deficiencies [6-8]: inrush current, which is easy to damage the devices of leg at startup. High capacitance voltage on impedance network during steady state, therefore large volume of capacitors are required and then the cost increases for this inverter. In addition, due to the shootthrough zero vectors replace part of traditional zero vectors, so the circle synthetic by SVPWM is not so smooth and generating the effect of output AC waveform. So aiming at the deficiencies of traditional Z-source inverter, other Z-source inverter topologies are analysed and advantages and disadvantages as well as application of them are summarized. 2. Circuit characteristics analysis of all kinds of Z-source inverters Z-source inverter consist of passive network and three-phase inverter. Z-source inverter works in nine states of switch including six effective vector states, two traditional zero vector states and one shootthrough zero vector state. When the Zsource inverter works in six effective vector ELECTROTEHNICĂ, ELECTRONICĂ, AUTOMATICĂ, 63 (2015), nr. 3 34 states, inverter leg is equivalent to a current source. When the Z-source inverter works in traditional zero vector state, inverter leg is regarded as the current source whose current value is zero. When the Z-source inverter works in shoot-through zero state, inverter leg is short-circuited. SVPWM modulation strategy is used in this paper to make the upper and lower devices of inverter leg turn-on and turn-off. Compared to SPWM modulation strategy, it has the advantages of high DC voltage utilization, fast dynamic response, less harmonic and fluctuation [9]. The following Z-source inverter topologies are understood to be ideal ones. T1 is a shoot through interval in a switching cycle, T 2 is a non-shoot-through interval in a switching cycle i.e. the switching cycle T = T 1 + T 2. 2.1 Traditional Z-source inverter Traditional Z-source inverter is shown in Figure 1 [10]. V C1 L1 D C1 U dc C2 VT6 VT4 i1 c VT2 L2 Figure 1. The topological structure of the traditional z-source inverter Assuming capacitors C1 and C2 and inductors L1 and L2 are identical, because of symmetry Z-source network, we have: C1 = C 2 = C L1 = L 2 = L (1) Then we can can write: VC1 =VC2 =VC (2) V L1 = V L 2 = V L The equivalent circuits of traditional Zsource inverter, which operates in shootthrough zero vector state and non shootthrough state are as shown in Figure 2. V L1 VC 2 i1 b uc VL1 C2 i1 a ub Vi L1 VC1 VT5 ua L1 dc VT3 VT1 V Vi C1 C2 VC1 VC 2 Vi = 0 dc VL 2 VL2 L2 L2 (a) equivalent circuit of non-shoot-through state (b) equivalent circuit of shoot-through state Figure 2. State equivalent circuit diagrams of the traditional Z-source inverter By analysing the state figures of the above equivalent circuit, Z-source inverter operates in non-shoot-through state and diode is turn-on, there are: according to equation (2) to (4), we have: Vdc=VL+VC Vi = VC − V L = ,V = V i C − VL = 2VC − Vdc (3) When the traditional Z-source inverter operates in through state, the diode is turnoff, there are: VC=VL , V =0 (4) i In steady state, based on the inductor voltage volt-second theorem, the average value of inductor voltage in a switching cycle is equal to zero. Therefore, we can write: − VL = T1V C + T 2 (V dc − V C ) = 0 T Assuming T1 = D1 T , T2 = (1 − D 1 ) T (5) , and VC = T2 1 − D1 V dc = V dc T2 − T1 1 − 2 D1 ∧ 1 Vdc = BVdc 1 − 2 D1 (6) (7) where, D1 is shoot-through duty cycle, Vdcis ∧ input DC voltage, V i is the peak DC voltage across the inverter, B is boost factor. The dotted line in Figure 1 is the circuit of inrush circuit flowing when traditional Zsource starts working. This moment, capacitance of the capacitors in the Z-source network are about zero and inductive reactance is large enough, so the inrush circuit at startup is very large and easy to damage the devices. What’s more, resonance happens through the interaction between the captance and inductive ELECTROTEHNICĂ, ELECTRONICĂ, AUTOMATICĂ, 63 (2015), nr. 3 reactance, and thus make the system unstable. In addition, due to the energy storage elements does not connect directly with DC input voltage, so the current flowing into the three-phase inverter is discontinuous. Analysis of the following Z-source inverters are the same as the traditional Z- source inverter. All will be analysed during their shoot-through state and non-shootthrough state. 2.2 Quasi-Z-source inverters As shown in Figure 3[11], there are quasi Z-source inverters that are symmetric and asymmetric inverters. C1 C1 L2 V dc D C2 35 D L2 L1 V dc Vi (a) asymmetric quasi Z-source inverter topology L1 C2 Vi (b) symmetric quasi-Z-source inverter topology Figure 3. The topological structure of two kinds of quasi Z-source inverters For the asymmetric quasi Z source inverter, due to the energy storage element L being in series with input DC voltage, so current flowing into the three-phase inverter bridge is continuous. Contrary to the asymmetric Z-source inverter, current is interrupted for symmetric Z-source inverter. Aiming at asymmetric quasi-Z-source inverter, as shown in Figure 3(a), according to volt-second theorem, during the steady state, we have: VC1 = T1 D1 V dc = V dc T1 − T 2 1 − 2 D1 (8) VC 2 = 1 − D1 T2 Vdc = Vdc T2 − T1 1 − 2 D1 (9) Peak DC voltage across the inverter of the asymmetric quasi Z-source inverter can be written as: ∧ D 1− D1 1 Vi = VC1 +VC2 = ( 1 + )Vdc = Vdc = BVdc 1− 2D1 1− 2D1 1− 2D1 (10) As to symmetric quasi-Z-source inverter, consider Figure 3(b), we can write: VC1 = VC 2 = T1 D1 Vdc = Vdc T1 − T2 1 − 2 D1 ∧ Vi = 2VC −Vdc = T 1 Vdc = Vdc = BVdc T2 −T1 1−2D1 (11) (12) As can be seen from above analysis, impulse current can be amortized and suppressed for quasi Z-source inverters owing to their energy storage inductor, which is in series with their Z-source passive impendence networks. However, they still give rise to the inductor current and capacitor voltage exceed the steady state value after startup of quasi Z-source inverter. Starting impulse current the start flowing inductor current and voltage across the capacitor exceeds the steady state value and resonance oscillation may take place for inductor and capacitor in the Z-source impendence network, then affect the stability of the system. From formula (9), it can be seen that at the same shoot-through duty ratio, the capacitance of capacitor voltage is less than the traditional Z source inverter during the steady state, and thus the side and weight of the capacitors can be reduced for this topology. Because reverse blocking effect of the diode, there is no in rush current at startup start and the stability and reliability of the system can be improved. Two kinds of quasi Z-source inverters have the same boost capacity as traditional Zsource inverter. In addition, traditional zero vector is inserted into through zero vector to realize boost for two quasi Z-source inverters, so two zero vector are coupled with each other and the waveform of output voltage is affected with modulation strategy in SVPWM. 2.3 Improved Z-source inverters Two kinds of modified Z-source inverters are shown in Figure 4[12]. ELECTROTEHNICĂ, ELECTRONICĂ, AUTOMATICĂ, 63 (2015), nr. 3 36 V dc L1 V dc Vi C1 C2 D V i L2 (a) Improved Z-source inverter 1 (b)Improved Z-source inverter 2 Figure 4. The topological structure of two kinds of improved z-source inverters The position of their Z-source impedance networks relative to three-phase inverter bridge is different from the traditional one. Consider Figure 4 based on inductor voltage volt-second theorem, the capacitor voltage and peak DC voltage across the inverter are expressed as: VC = ∧ Vi = D1 V dc 1 − 2 D1 (13) 1 V dc = BV dc 1 − 2 D1 (14) of output voltage is affected modulation strategy SVPWM. with 2.4 Enhanced Z-source inverters Enhanced Z-source inverters are divided into two types including improving boost capacity and reducing capacitor voltage ones in steady state. In order to improve boost capacity of Z-source inverter and further reduce its capacitor voltage during steady state. Several enhanced Z-source inverters were proposed. They were added impedance network and passive switching devices to form enhanced Z-source topologies. All of them are listed as follow. As can be seen from above formulas, the capacitor voltage and peak DC voltage across the inverter are the same as symmetric quasi Z-source inverter. What’s more, The method of boost for improved Z-source inverter is similar to the symmetric quasi Z-source inverter, so it still remains the same shortcoming that two zero vector are coupled with each other and the waveform 2.4.1 Enhanced Z-source inverter of improving boost capacity Enhanced Z-source inverters of improving boost capacity [13] are presented in Figure 5. D2 C2 C1 L3 D 3 V dc C3 D L2 L3 D 3 L1 V dc C2 C3 C1 D L2 C4 Vi (a) Enhanced Z-source inverter with auxiliary diodes D4 D12 D5 L3 L1 D1 C1 Vi (b) Enhanced Z-source inverter with auxiliary capacitors L2 D3 D2 C2 D V dc L1 Vi D6 L4 D D8 7 L5 D11\ D9 D 10 \ L6 (c) Enhanced Z-source inverter with switching inductors Figure 5. Enhanced z-source inverters of improving boost capacity As shown in Figure 5(a), this topology, called diode auxiliary enhanced Z-source inverter, is added diodes D2 D3, inductor L3 and capacitor C3. Over the symmetric quasi Z-source inverter to form boost chopper circuit. It is in series with three-phase inverter bridge to improve boost capacity and make sure continuous input current into ELECTROTEHNICĂ, ELECTRONICĂ, AUTOMATICĂ, 63 (2015), nr. 3 three-phase inverter bridge. Diode D2 of the topology in Figure 5 (a) is eliminated and added capacitor C2 instead, so we can get capacitor auxiliary enhanced Z-source inverter, which is shown in Figure 5(b). Due to the increase of energy storage element C2, boost capacity of this topology is better than that of the topology in Figure 5 (a) and current inputting into three-phase inverter bridge of this topology is continuous else. As shown in Figure 5 (c), the switching inductive Z-source inverter technology is added several switching inductive energy storage elements to further reinforce its boost capacity, but due to the absence of the energy storage element in series with input DC voltage, so input current is discontinuous. It is worth mentioning that three enhanced Z-source inverters mentioned above have extensibility features and then corresponding impedance networks and diodes can be aggrandized to increase their boost capacity. Besides, impulse currents at startup for them does not exist. 2.4.2 Enhanced Z-source inverter of reducing capacitor voltage during steady state Enhanced Z-source inverters of reducing capacitor voltage during steady state are listed as follow[14]: The following enhanced topologies further reduces capacitor voltage stress during steady state. As can be seen in Figure 6(a), the enhanced Z-source inverter topology in the traditional Z-source inverter based on the DC input voltage is dived into two that are respective in series with the inductor branches in the impedance network. Vdc / 2 C1 L1 C1 D L2 C2 L1 C2 V dc Vi Vi D 37 C3 D1 L3 L4 Vdc / 2 C4 (a) Enhanced Z-source inverter with embedded DC power (b) Enhanced Z-source inverter with tandem quasi-z network C1 D L2 L1 C2 V dc Vi C3 L3 D1 L4 C4 (c) Enhanced Z-source inverter with coupled quasi-z network Figure 6. Enhanced z-source inverters of reducing capacitor voltage stress It keeps symmetric for Z-source inverter and decreases ripple current flowing through DC power source as well as the capacitor voltage stress during steady state by a factor of two. Due to no adding energy storage element, boost capacity is unchanged for this topology. Enhanced Z-source inverters, which are respectively added symmetric and asymmetric quasi Z-source inverters are shown in Figure 6(b) and (c). The topologies both have continuous input currents and lower capacitor voltage stress during steady state, so small-sized, light-weighted and low-cost capacitors can be used in the two topologies. Since there is no increase of energy storage elements in the impedance network, boost capacity of three inverters mentioned above are remain unchanged. Because boost capacity of all enhanced Z-source inverters is increased by putting their shoot-through zero vector replace partial even all traditional zero vectors and two kinds of zero vectors are coupled ,quality of output voltage can be affected in SVPWM. ELECTROTEHNICĂ, ELECTRONICĂ, AUTOMATICĂ, 63 (2015), nr. 3 38 Figure 7(a) and (b) show Two kinds of IST(Isolated Shoot-Through) Z-source inverters. 2.5 Isolated shoot-through Z-source inverters Vi Vi (a)Isolated shoot-through Z-source inverter 1 (b) Isolated shoot-through Z-source inverter 2 Figure 7. Topological structure of shoot-through inverters Based on improved Z-source inverter, two topologies are added controlled device IGBT to control the insertion of shoot-through zero vector solely, and thus effectively solve the coupling between shoot-through zero vector and traditional zero vector. In addition, a large capacitor Cu is used to suppress the fluctuation of DC bus and supply sudden large amounts of current. In order to inhibit discharging of the large capacitor through IGBT, diode VDS is needed. Due to solving the coupling between shoot-through zero vector and traditional zero vector, IST Z-source inverter has higher quality output AC voltage[15]. Summarizing boost factors and capacitor voltages during steady state of all Z-source inverters and enumerating them in the table below: Table 1. Comparison in properties of 13 kinds of Z-source inverter in properties Enhanced Z-source inverters Enhanced one with auxiliary diodes boost factor capacitor voltage during steady state/V 1/[(1− D1)(1− 2D1)] Vdc /[2(1 − 2D1 )(1 − D1 )] Enhanced one of auxiliary capacitors 1 /(1 − 3D1 ) Vdc /[3(1 − 3D1 )] Enhanced one with switching inductors (1+2D1)/(1−4D1) Vdc (1 − D1 ) /(1 − 4 D1 ) Enhanced one with embedded DC power 1 /(1 − 2D1 ) Vdc (1 − D1 ) /[2(1 − 2D1 )] Enhanced one with tandem quasi-z network 1 /(1 − 2D1 ) Vdc (1 − D1 ) /[2(1 − 2D1 )] Enhanced one with coupled quasi-z network 1 /(1 − 2D1 ) Vdc (1 − D1 ) /[2(1 − 2D1 )] Isolated shoot-through one 1 /(1 − 2D1 ) Vdc /(1 − 2 D1 ) 3 MATLAB Using MATLAB software for all Z-source inverters mentioned above to conduct simulations. Shoot-through duty ratio D1 is taken as independent variable on the horizontal axis, ratio of capacitor voltage during steady state and DC power voltage V C / V dc is used as dependent variable. Besides, boost factor B is also regards as dependent variable on the vertical axis. Simulation results are as follows. ELECTROTEHNICĂ, ELECTRONICĂ, AUTOMATICĂ, 63 (2015), nr. 3 39 3 2 1.8 2.5 1.6 2 1.2 VC / Vdc VC / Vdc 1.4 1.5 1 0.8 1 0.6 0.4 0.5 0.2 0 0 0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0 0.05 0.1 0.15 (a) 0.25 0.3 (b) 15 10 10 B B 15 5 0 0.2 D1 D1 5 0 0.05 0.1 0.15 0.2 0.25 0 0.3 0 0.05 0.1 0.15 D1 0.2 0.25 0.3 D1 (c) (d) Figure 9. Boost capacity and capacitor voltage during steady state of all kinds of Z-source inverters From the above simulation results, we can know switching inductive enhanced Z-source inverter has the best boost capacity of all, enhanced Z-source inverter of DC power embedded, coupled network and trandem type have the lowest capacitor voltage during steady state. 4. Control strategy There are several space vector pulse width modulation techniques used for Zsource inverters to control the connection and break of switch devices in three-phase inverter bridge. The control strategies are listed as follow [15-18]: (1) Simple SVPWM Boost Control Strategy (2) Maximum SVPWM Control Strategy (3) Shoot-through State segmented SVPWM Boost Control Strategy For Simple SVPWM Boost Control Strategy and Maximum SVPWM Control Strategy, partial traditional zero vectors or all traditional zero vectors are replaced by shoot-through zero vectors to realize boost, but switching frequency is increased and Zsource system’s efficiency is reduced. For Shoot-through State segmented SVPWM Boost Control Strategy, shoot-through zero vectors which are distributed equally to each phase leg to balance the loss of electrical current are inserted during commutation, so switching frequency of switching devices remains unchanged and the system has higher efficiency. In conclusion, we choose it to control the connection and break of the switching devices of each phase leg. Figure 10(a) and (b) shows the control theory of SVPWM. (T − T3 − T2 ) / 4 T2 / 2 T3 / 2 (T − T3 − T2 ) / 2 β T3 / 2 T2 / 2 (T − T3 − T2 ) / 4 U 6 (110) U 2 (010) U ref U 3 (011) U1 (001) U 4 (100) α U 0 (000) U 7 (111) U 5 (101) T1 / 6 Figure 10. Control theory of SVPWM Only analysing the first sectors in this paper, other sectors have the same analytic ELECTROTEHNICĂ, ELECTRONICĂ, AUTOMATICĂ, 63 (2015), nr. 3 40 approach. U1~U6 are six active vectors, U0 (000) and U7 (111) are traditional zero vectors, Uref is a of reference voltage vector of synthesized by two active vectors. By controlling the connection and break, these eight vectors are produced and they approximate a flux linkage cycle. At last, high output-quality voltage waveform in inverter of inverter’s AC side is generated. This vector is through the eight-leg switches control to produce, and thus take advantage of the eighth flux vector to approximate the circle and then the output waveform of the inverter’s AC side. 5. SIMULINK All topologies are simulated in MATLAB along with Simulink and SimPower Systems Toolbox. According to the relationship between modulation ratio m and shoot- through duty ratio D1: D1 = T1 = 1 (2 − 3m) T 2 [19-20]. Assuming m=0.8, we have D1 = 0.307 . Other simulation parameters can be also set: Vdc=200 V, the capacitance of capacitor and inductance of inductor are decided by inhibiting the ripple current of inductor and ripple voltage of capacitor, different topologies have different capacitances and inductances. Simulink based simulations are shown in Appendix 1 (Figure) including output phase voltages and output line voltages as well as input currents of all kinds of Z-source inverter mentioned above. Summarizing the properties of all Zsource inverters and enumerating them in the table below. Table 2. AC output voltages conparison of 13 kinds of Z-source inverter in properties Enhanced Z-source inverters Traditional one Asymmetric quasi one Symmetric quasi one Improved one Enhanced one with auxiliary diodes Enhanced one with auxiliary capacitors Enhanced one with switching inductos Enhanced one with embedded DC power Enhanced one with tandem quasi-z network Enhanced one with coupled quasi-z network Isolated shoot-through one Phase voltage/V 210 210 210 210 280 310 390 210 210 210 210 As can be seen from Table 1 and Figure 8, traditional Z-source inverter has limited boost capacity, larger and discontinuous input current and higher capacitor voltage during steady state. Aiming at overcome the deficiencies of traditional Z-source inverter. Other Z-source inverters show them in different ways. For reducing the capacitor voltage during steady state, Z-source inverters in Appendix 1 (h), (i), (j) have the lowest capacitor voltages of all during steady state, but two of them,enhanced DC power embedded and enhanced quasi trandem Zsource inverter, have the discontinuous input currents. Besides, these three topologies costs increases. Aiming at boost capacity, Z-source inverters in Appendix 1(e), (f), (g) have the better boost capacity. Thereinto, switching inductive Z-source inverter has the best boost capacity of all, but its input current is discontinuous and it still has the incrush Line voltage/V 350 350 350 350 470 520 580 350 350 350 350 input current/A 205 (discontinuous) 310 (continuous) 340 (discontinuous) 430 (discontinuous) 410 (continuous) 270 (continuous) 520 (discontinuous) 260 (discontinuous) 280 (discontinuous) 220 (continuous) 310 (continuous) current at startup. What’s more, costs for these three Z-source inverters increases much. As to improved Z-source inverters, quasi Z-source inverters and shoot-through Zsource inverters. Appendix 1(b), (c), (d), (k) show their simulation results that they have lower capacitor voltages than traditional Zsource inverters and incrush currents does not exist in them. In addition, these three topologies are more economic than other topologies. Last but not the least,the quality of output voltage including output phase voltage and output line voltage for isolated shoot-through Z-source inverter is the best due to its shoot-through zero vectors inserted solely by IST-IGBT. Overall, isolated shoot-through Z-source inverter has the best property of all. 6. Conclusions Aiming at the disadvantages of traditional Z-source inverter, analysis and research are ELECTROTEHNICĂ, ELECTRONICĂ, AUTOMATICĂ, 63 (2015), nr. 3 conducted for the structural principle of other kinds of Z-source inverters in this paper. By comparing with other Z-source inverters in their properties including boost capacitor,capacitor voltage during steady state, input current of three-phase inverter bridge, no incrush current at startup, the overall performance of isolated shootthrough Z-source inverter is the most excellent. According to the conclusion of this paper, isolated shoot-through Z-source inverter will be used in permanent-magnet direct-driven wind power system next due to its wide application and limited localization a) A traditional one 41 with photovoltaic power generation,wind power generation and fuel cell technology pullulating. 7. Acknowledgements This work is supported by the National Natural Science Foundation of China (Grant No.61263004) and Gansu Province Natural Science Foundation (Grant No.1212RJZA071). 8. Appendix 1 AC Output voltage of all kinds of Z-source inverters are presented as follows: b) An asymmetric quasi one (c) A symmetric quasi one (d) An improved one (e) An enhanced one with auxiliary diodes (f) An enhanced one with auxiliary capacitors (g) An enhanced one with switching Inductors (h) An enhanced one with embedded DC power (i) An enhanced one with tandem quasi-z network 42 ELECTROTEHNICĂ, ELECTRONICĂ, AUTOMATICĂ, 63 (2015), nr. 3 (j) An enhanced one with coupled quasi-z network 9. References [1] X. Zhang, C.W. Zhang, PWM rectifier and its control, Beijing: Machinery industry press, 2012. [2] L. Zhou, L.Q. Zhang, B. Liao, “Research on control Strategy of single phase photovoltaic inverter”, Power SystemTechnology, 2012, 36(9), pp. 25-30. [3] B. Cui, Z.M. Qian, X.P. Ding, F.Z .Peng, “A voltage-current close loop control algorithm forZ-source inverter, Power Electronics, 2007, 41(9), pp.1-3. [4] J.Z. Dou, “Study on intelligent gridconnected Controller for offshore wind power system”. Harbin Institute of Technology, 2012, pp.11-19. [5] Q. Gao, Z.M. QIian, B. Gu, “An abnormal operatingState analysis of Z-source inverter”. Transactions of China Electrotechnical Society, 2005, 20(8), pp55-58. [6] X.P. Ding, Z.M. Qian, B. Cui, F.Z. Peng, “A High-performance Z-source inverter operating at wideRange load”. Transactions of China Electrotechnical Society, 2008, 23(2), pp.61-67. [7] K. GUO, H.X. Li, L. Zhou, “Implementation of single Phase Z-source inverter grid-connected system based on inductor current control”. Power System Protection and Control, 2012, 40(23), pp.68-72. [8] F.Z. Peng, “Z-souce inverter”, IEEE Transactions on Industry Applications, 2003, 39(2), pp.504-510. [9] S.T. Yang, X.P. Ding, F. Zhang, Z.M. Qian, “Study on Z-source inverter for photovoltaic generation system”, Proceedings of the CSEE, 2008, 28(17), pp.112-118. [10] L.J. Zhang, G.J. Tan, L.P. Chen, “Neutralpoint potential balance control for threelevel Z-source inverters based on double modulation wave technique”, Power System Protection and Control, 2013, 41(7), pp.9196. [11] Y. Li, F.Z. Peng, “Constant capacitor (k) An isolated shoot-through one voltage control strategy for Z-source/quasi Zsource inverter in grid-connected photovoltaic systems”, Transactions of China ELectrotechnical Society, 2011, 26(5), pp.6269. [12] B.C. Xue, X.P. Ding, C.H. Zhang, M. Zhang, “Quasi Z-source inverter adjustable speed drives system and its partly PAM/PWM control strategy”, Transactions of China Electrotechnical Society, 2012, 27(10), pp.142-149. [13] Y. Tang, S.J. Xie, C.H. Zhang, “Improved Z-source inverter”, Proceedings of the CSEE. 2009(30), pp.28-34. [14] Y.F. Zhou, W.X. Huang, J.W. Zhang. “A high gain Z-source inverter”, Transactions of China Electrotechnical Society, 2013, 28(9), pp.239-246. [15] Y.F. Zhou, W.X. Huang, J.W. Zhao, “Tapped inductor quasi Z-source inverters”, Proceedings of the CSEE, 2012, 32(27):126133. [16] C.W. Cai, Y.B. Qu, K. Sheng, “Improved maximum constant boost control of Z-source inverter”, Electric Machines and Control, 2011, 15(12), pp.14-20. [17] Vinnickov D., Roasto I., “Quasi-Z-SourceBased Isolated DC/DC converters for Distributed Power Generation”, IEEE Trans.Ind.Electron, vol.58, no.1, pp.192-201, Jan.2011. [18] P.C. Loh, D.M. Vilathgamuwa, Y.S. Lai, G.T. Chua, Y.W. Li, “Pulse width modulation of Z-source inverters”, IEEE Trans power Electron. 2005, vol.20, pp.1346-1355. [19] X. Liu, P.C. Loh, P. Wang, X. Han, “Improved modulation schemes for indirecr Z-source matrix converter with simusoidal input and outputwaveforms”, IEEE Trans Power Electron, vol.27, no.9, pp.4039-4050, Sep.2012. [20] M. Zhu, K. Yu, F.L.Luo, “Switched-inductor Z-source inverter”, IEEE Trans. Power Electron, vol.25, no.8, pp.2150-2158, Aug.2010. ELECTROTEHNICĂ, ELECTRONICĂ, AUTOMATICĂ, 63 (2015), nr. 3 10. Biography Hongsheng SU was born in Jingyuan (China), on November 1969. He graduated from Lanzhou Jiaotong University, Electrical Engineering and Automation in Lanzhou (China), in 2001. He received the PhD degree in Power Systems and Automation from Southwest Jiaotong University of Chengdu (China). He is Professor at the Lanzhou Jiaotong University, in Lanzhou (China). His research interests concern: Automatic control and reliability engineering, System Security and Reliability, grid-connected wind power system based on Z-source inverter and its gridconnected control, Power Systems and Its Automation. Correspondence address: School of Automation and Electrical Engineering, Lanzhou Jiaotong 43 University, Anning West Road No.88, Anning District, Lanzhou, Gansu, China, 730070, e-mail: lhj41333696@163.com Hongjian LIN was born in Hai nan (China), on November 1990. He graduated from Lanzhou jiaotong University, Electrical Engineering and Automation in Lanzhou (China), in 2013. He received the bachelor’s degree in electrical engineering and the automatization specialty from Lanzhou jiaotong University of Lanzhou (China). He is a postgraduate in Lanzhou jiaotong University, in Lanzhou (China). His research interests concern: grid-connected wind power system based on Z-source inverter and its grid-connected Control as well as power system and Automation.