International Journal of Engineering Trends and Technology (IJETT) – Volume 12 Number 10 - Jun 2014 Space Vector PWM Implementation for Z-Source Inverter K Veera Reddy1 M Vinod2 M Niranjan3 M Durga Raj4 A V Ravi Kanth K5 Dept. of EEE, KLUniversity, Vaddeswaram, Guntur, A.P., India Abstract: Space Vector Modulation (SVM) Technique has become the most popular and important PWM technique for three phase Voltage Source Inverters. Z-Source Inverters have the ability to boost the dc link voltage, thus increasing the output ac voltage beyond the values reached by conventional inverters. The enhanced ratio from ac output voltage to dc link voltage is possible due to an impedance network connected between the dc power supply and the main converter. This paper presents implementation of Space Vector Modulation technique for Two Level Z Source Inverter using MATLAB. Keywords: Z source inverter, Space vector PWM, impedance network, dc bus utilisation. I. INTRODUCTION Space Vector modulation (SVM) technique was originally developed as a vector approach to pulsewidth modulation (PWM) for three-phase inverters[1].It is a more sophisticated technique for generating sine wave that provides a higher voltage to the motor with lower total harmonic distortion. It confines space vectors to be applied according to the region where the output voltage vector is located. A different approach to PWM modulation is based on the space vector representation of voltage in the α-β plane. The α-β components are found by transformations [2][4]. The determination of switching instant may be achieved using space vector modulation technique based on the representation of switching vectors in α-β plane. The Space vector modulation technique is an advanced, computation intensive PWM technique and is possibly the best among all the PWM techniques for drives applications. Because of its superior performance characteristics, it is been finding wide spread application in recent years [5],[6]. The purpose of this paper is to present the space vector modulation technique and then to simplify the explanation of how it can be implemented using software packages. II. FEATURES OF SPACE VECTOR PWM The main aim of any modulation technique is to obtain variable output having a maximum fundamental component with minimum harmonics. During the past years many PWM techniques have been developed for letting the inverters to posses various desired output characteristics to achieve the following aim: ISSN: 2231-5381 wide linear modulation range Less switching loss. Lower total harmonic distortion. The space vector modulation (SVM) technique is more popular than conventional technique because of the following excellent features: o o o o o o o o o It achieves the wide linear modulation range associated with PWM third-harmonic injection automatically. It has lower base band harmonics than regular PWM or other sine based modulation methods, or otherwise optimizes harmonics. 15% more output voltage then conventional modulation, i.e. better DC-link utilization. More efficient use of DC supply voltage. SVM increases the output capability of SPWM without distorting line-line output voltage waveform. Advanced and computation intensive PWM technique. Higher efficiency. Prevent un-necessary switching hence less commutation losses. A different approach to PWM modulation base don space vector representation of the voltages in the α-β plane. III. Space Vector concept The concept of space vector is derived from the rotating field of AC machine which is used for modulating the inverter output voltage. In this modulation technique the three phase quantities can be transformed to their equivalent 2-phase quantity either in synchronously rotating frame (or) stationary frame. From this 2-phase component the reference vector magnitude can be found and used for modulating the inverter output. The process of obtaining the rotating space vector is explained in the following section, considering the stationary reference frame. Let the three phase sinusoidal voltage component be, Va =Vm sin wt Vb =Vm sin (wt-2π/3) Vc =Vmsin(wt-4π/3) When this 3-phase voltage is applied to the AC machine it produces a rotating flux in the air gap of the AC machine. This rotating flux component can be http://www.ijettjournal.org Page 499 International Journal of Engineering Trends and Technology (IJETT) – Volume 12 Number 10 - Jun 2014 represented as single rotating voltage vector. The magnitude and angle of the rotating vector can be found by mean of Clark’s Transformation as explained below in the stationary reference frame. The representation of rotating vector in complex plane is shown in Figure 1[7] Solving the above two simultaneous equations, one gets: T1 | v sr | Ts sin( / 3 ) Vdc sin( / 3) T2 | v sr | Ts sin Vdc sin( / 3) |Vsr| represents the length of the reference Vector and is measured from the start of the vector. 4) Assert the appropriate control signals to affect the required switching action. Figure 1.Representation of Rotating Vector in Complex Plane A. Realization of Space Vector PWM 1) The sector in which the tip of the reference sector is situated is to be determined from the instantaneous phase references Va *, Vb * and Vc* Va *, Vb *, Vc * The three pahse voltages are transformed to two phase using parks transformation. vα,vβ Θ= tan-1(vβ/vα) α = Θ- k(600) ; k such that α< 600 Sector number = k + 1 2) Computation of T1 and T2; here lookup tables are needed to know the values of Sin (600- α) and Sin α 3) Determination of switching vectors. Using the corresponding sector information the actual switching time for each inverter leg is generated from the combination of effective times and zero sequence time. Equating volt-seconds along the α -axis: (ІVsrІcosα)* Ts = Vdc *T1 + (Vdccos60 0) * Ts Equating volt-seconds along the β -axis: (ІVsrІsinα) * Ts = (Vdcsin600) *T2 ISSN: 2231-5381 Fig.2 Switching sequence sector 1[8] http://www.ijettjournal.org Page 500 International Journal of Engineering Trends and Technology (IJETT) – Volume 12 Number 10 - Jun 2014 The sequences varies from one sector to the other sector capacitance, the order of the differential equations can be reduced in two. The state variables of the intermediate circuit are iz and v z. The inverter is a two-level VSI formed by six IGBTs. The load is a three phase RL circuit. Fig3 Space vector pwm simulation block IV. Z SOURCE INVERTER Voltage Source Inverters (VSI) controlled by Space Vector Modulators (SVM) produce output voltages whose fundamental amplitude is given by[9] Vs = * Vdc Fig.4 Z source three phase VSI V. SIMULATION RESULTS √ Where M- modulation index Vdc- DC link voltage The maximum amplitude is given by Vs = √ = 0.57*Vdc when m=1 On the other hand, Z-Source Inverters (ZSI) produce output voltages that are higher than those obtained by the Voltage source inverter Vzs,max > Vs,max with the same VDc. This is the main advantage of this configuration. The intermediate circuit of the ZSI is composed by two inductors, L z, two capacitors , and a diode D z, see Fig. 2. Assuming that both inductors have the same inductance, and both capacitors have the same ISSN: 2231-5381 Fig.5 Three phase voltages of Z-Source inverter http://www.ijettjournal.org Page 501 International Journal of Engineering Trends and Technology (IJETT) – Volume 12 Number 10 - Jun 2014 vector pwm is implemented for z source inverter. The z impedance network when used in gives desired output voltage and harmonic content is reduced. The space vector is implemented and corresponding results low harmonic distortion, more dc bus utilization are observed. REFERENCES Fig.6 THD Analysis of Z-source inverter voltages CONCLUSION The DC bus utilisation is increased by space vector pulse width modulation. In this paper space ISSN: 2231-5381 [1] H. W. v. d. Brocker, H. C. Skudenly, and G. Stanke, “Analysis and realization of a pulse width modulator based on the voltage space vectors, “in Conf. Rec. IEEE-IAS Annu. Meeting, Denver, CO, pp. 244–251, 1986. [2] O. Ogasawara, H. Akagi, and A. Nabel, “A novel PWM scheme of voltage source inverters based on space vector theory,” in Proc. EPE European Conf. Power Electronics and Applications, pp. 1197– 1202, 1989. [3] D. Jenni and F. Wueest, “The optimization parameters of space vector modulation,” in Proc. 5th European Conf. Power Electronics and Applications, pp. 376–381, 1993. [4] S. R. Bowes and Y. S. Lai, “The relationship between spacevectormodulation and regular-sampled PWM,” IEEE Trans. Power Electron., vol.14, pp. 670–679, Sept. 1997. [5] J.-H. Youm and B.-H.Kwon, “An effective software implementation of the space-vector modulation,” IEEE Trans. Ind. Electron., vol. 46, pp.866–868, Aug. 1999. [6] Zhou and D. Wang, “Relationship between space-vector modulation and three-phase carrier-based PWM: A comprehensive analysis,” IEEE Trans. Ind. Electron., vol. 49, pp.186–196, Feb. 2002. [7] D.Rathnakumar and J.LakshmanaPerumal, T.Srinivasan “A New Software Implementation of Space Vector PWM” IEEE Trans. Ind. Electron., vol. 59, pp.1186–1196, Feb. 2005. [8] BengiTolunay”Space Vector Pulse Width Modulation for ThreeLevelConverters - a LabVIEWImplementation”,UPTEC E12001 [9] N. Muntean, L. Tutelea, I. Boldea “A Modified Carrier – Based PWM ModulationTechnique in Z - Source Inverters” IEEE Trans. http://www.ijettjournal.org Page 502