ACTIVE FILTICIIS SIMULATION TO CORRECT TkE POWER FAC1I~OIP USING PSPICE. Rtt-r-icioSalmer6n Revuelta (I' Juan C. Montan0 Asquerino (z Dept. Fisica Aplicada e Ingcni8:ria ElCctrica. University d Huelva, Escuela Politecnica Superior. Ctra. Palos dc la Frontcra. 21819 La Rabida, Huelva, Spain. F'hone (+34) 59 350651 Fax (+34) 59 350311 Email: Patricio@uhu.es IRNA, Consejo Superior de Invcstigaciones Cientiilicas. AV&. Reina Mcrccdcs s/n. 41012 Scvilla, Spain. (+34) 54 624711 Fax (+34> 54 624M2 Email: MontarioI@cica.es Abstract.-The fundamental re:sults of the instantaneom power theory have been applied to optimize the power factor iii three-phase systems with nonlinear loads. Compeiisa(ion in steady and transient state:; is considcred. The mtd& for PSPICE oE an active poww i[ilter and a control circuit arc presented. The results of a pr.aclica1case, using these , A&" are included. I. b!TRODUCTION The current nccd of correcting the power factor in Three-phase system with iionlinear loads has motivated, UI the recent years, the appearance of a great i i u " of projects on static VAr compensators [l]. Sincc the 80's concrctcly, electrical engineers have bccn investigating tho utilization of so-called de5,igilatcd active power f i l t e r s for the compelsation of three-phase nonlinear loads, sucli a!< rectifiers, AC choppers a d cycloconverters [2-81. Active power filters ate based on a DC-AC bridge convertcr, with fed-in voltage or current, constituted by switching deviccs with practically no energy storagc componeiits. At present, d-e switching elements are of thc types BITS, MOSFETS ard IGBTS, tllat switch incrmsetl currents in very short times with high performance. Pulsc Width Modulation (P'YM) techniques are generally use to control the converter [3-51 This permits injection into thc electrical line of a sequcncc: of current pulses with differctit objectives, such as optim~zation of the power factor. In such case, the objectivc is to obtain a line-curmilt waveform that rcpruduces t h a supply voltage waveform. This paper approaches the problem of compcnsating three-phase nonlincar loads in sinusoidal and nonsinusoida I situations with the objective of developing a i n d e l of active power filter aid its control circuit, to verify theoretical predictions and system perfonnancc tlxough simulated tests, facilitating the coniputcr presentation of the waveforms of interest. The module analog Deliaviornl nrodcling provides great wsatility for tlie simulation of bolck diagrams. These characteristics make PSPICE an especially interesting tool 1-01the analysis of active powcr filters. definition of two orthogonal components of the line current, i The f i s t is tlie mstc,inkuzeous active current, ip,and die second the znstatuneous rr'actwe current, i,,; of the two, oidy the fornicr is necessary for tlic transmission of the imtantaiieous power p('t).Thus, the current compcment i, is comlxmable. So, it is possible to speak of a truc process of ins[anfnneouscoinpensalion for a transient state. This IS exclusive of systcnis of more rhan one pliasc arid it represents conccptuall!: a novelty. Tlic complctc for~tnulatioriof thc problem is I-~rescntcd in (9-101. If the 3-plxise voltage-sourcc have a refermce such tlnt xu,= 0, th:: vector corresponding to the load current is dccomposcd in the fonn J = J P 4 where U is the insiantaieous voltage vector; U the instantaneous norm of U: J= Edn;p(t) the conventional instantaneous power: p= U'.< and io the instantaneous zcrophase sequence curremivector: io= LE, , where I = [111], aid 3.b= i,+i2+i3. For supplying the mstantaneous power to the load, oiily die current i, is necessary. So, to reduce t!ie line losses as: much as possible without altcrhg the ltt,tantawous power (or tlie iilstanta neous active a " u t ) transmission, that is, without using eiiergy storsge, the instantme ous nonactive current i, should be eliminated. The compensator can bc built with switching deyiccs without reactive elements, 111 this way its incoming instantaneous power is null arid it docs not interfere in die process of instantaneous t r a d e r of energy between source and load. Figure 1 shows the basic scheme of thc instantaricous compensation (3), (3) 11. INSTANTANEOUS AND STEADY STATE COMP.ZNSATION In tliree-phxe systemu, for arbitrary voltage ai01 current wavcfonns, the global process of energy exchangc bctwccn source and load I:, explained satisfactorily by tlic 0-7803-31-09-5/96/$5 00 + i Tliey are calculated instantaneously without any time delay by using the iilstantaneous voltages and currents on the load sidc . 1906 IEEE 1543 - 1 it el i3 I c2 U- 1 U- J 2 -I U- I I -I 3 0 Fig. 3. Active power filter. Fig. 1. Block diagram for the calculation of the instantaneous compensating current for a three-phase system. The circuit operates without the aid of energy storage elements. The coinpcnsating current is obtained by hysteresis control. The width of the hysteresis band is preset when the reference current is calculated. The discrete output levels of die hysteresis comparator determine die gating sequence of the switching devices, fig. 4. In the steady state one may be interested in studying the possibility of full compensation, i.e., the elimination of the non-active terms of the current to obtain unity PF. Under this condition, the voltage source supplies the active current dcfiicd by Fryze [ 1I], which means that the current source waveform reproduces the voltage source waveform. Fig.2 shows the block diagram for the calculation of reference waveforms for full compensation.. Two LPF are included for determination of die average power P and the average norm squared of the voltage (U') respectively. The quotient of both quantities constitutes the equivalent conductance (GJ .p I' Fig. 4. Hysteresis Control for one Phase. The converter output follows the reference waveform of the instantaneous reactive current, within the band imposed by the control operation. Several models of generalized power converters were simulated in a computer by using their transfer functions [12]. Thus, given the switching function matrix of the inverter (fig.5) and the voltage vector on the DC and AC sides defined respcctively by Fig. 2. Block diagram for calculating the full-compensating current. v, = [ v., v4 ; v, = [ v v., Sl . . . v.4] (4 and the respcctive current vectors, 111. ACTIVE POWER FILTERS: MODELS FOR COMPUTER-AIDED SIMULATION. The proposed type of compensator is the DC-AC converter which is shown in fig. 3 . It works as an active power filter that delivers the compensating current vector. The gating pulses switch the transistors of the three-phase bridge as usual and the output pulse amplitudes reach the voltage value of the DC side. the input-output rclatioilships are given by where A is the switching function matrix whose terms A, define the closed state "I", or the open state " 0 of the 1544 I LOAD I Fig. 7. Compcnsalcd three-phase bridgc controllld rectifier. Fig. 5. Switching matrix for multiphasc invcrter. switching element. Thus, it is vcrified It is assumed that this nodinear load is fed by a balanced sinusoidal SUI ply voltage. The switching elcmcnts SCRS of the rectifier are switched by a gating wip:lc of 60 dcg referred to the zero-crossing instant of the phase volt age. Fig. 8 shows significant waveforms of plase 11: source c m c n t before compensation, instantaneous compensating current and the compensatcd supply current. The last two prcscnt deviations with respect to thc rcfcrence signal (the shading region) due to the hysteresis band. and for the three-phase invccrtcr which enables establishmtnt of the equivalent circuit of dcpcndent sources (fig. 6), [12-13]. U A A : . . . . . . . :. ........... .! t + t Fig. 6 . Model for Computt:r-Aided Simulation of a ThreePhase Inverter. Each one of the elcmcnts of AV(') represents waveforms d c f i c d accoiding to two discrete levclls obtained on the output side of the hystcrcsis comparatoL, one per plase. This procedm constitutes the usual control of current by pulse widtli incldulation (PWM). a 1m. ................. ,................... .+.. IV. SIMULATION OF A PRACTICAL CASE. Thc principles set OUI in thc previous paragraphs on instantaneous and steady s t m compensation, as well as the methodology presented -01 obtaining computer-aided modcls of active jmwcr filters, are applied for the analysis of a practical case, 1141. Fig.7 shows a three-phase bridge rectifier with mductive load. b 1545 .................. *....................... -.* LOA ,................. +..................... .. delay equivalent to several fundTmenta1 periods of the supply voltage. Both can be implemented by using a static compensator built with the coilfiguration of a power inverter. The control system and the powcr circuit have been studied by using efficient computer models. These provide great versatility for the simulation of block ...... diagrams for control circuits using PSPICE. The simulation process makes it possible to confirm thc results on compensating load in different practical cases. torr; OR. -I(YXI TlCW REFERENCES C Fig 8 Waveforms Correspondmg to Phase 1 in the System Shown in fig 7 a) Current in Load, b) Instantaneous Compensating Current, c) Source Current after Compensation (11 T.J.E. Miller, "Reactive Power Control in Electric Systems" Fig. 9 shows the compensatiiig current and the source current after steady state compensation. .....:............ .-......... * i.L(,& 2ifl i. . . . . . . . . . . . . ..: . . . . . . . . . ............. ........5....................... .f + ~ ..... ,. . . . . . . .~ ?(XI I en< -,ru1 > <".r 1 lh.3 I',*% ili,i% xi- b Fig 9. a) Full Coinpcnsatmng Current b) Source Current after Compensation V. CONCLUSIONS For thrcc-phase systems and nonlinear loads, two different procedures of load compensation were considered: the instantaneous compensation, for eliminating the instantaneous reactive current, and the full conipensatzon, for eliminating all the non-active current components circulating through tlie load. The fist procedure is able to operate in the transient states. The second procedure is conceived only in steady shtes, the compensator suffers a John Wiley, 1982. [2] H. Akagi, Y . Kanazawa, and A. Nabae, "Instantanous Reactive Power Compensators Comprising Switching Devices Without Energy Storage Components", IEEE Trans on Industry Applications, vol.IA-20,No.3 pp 6 2 5 4 3 0 May/June 1984. [3] H. Akagi, A. Nabae, and S. Atoh, "Control Strategy of Active Powcr Filtcrs Using Multiple Voltage-Source PWM Converters", IEEE Trans. Iiid. Applicat., vo1.IA-22, no. 3, pp. 460-465, May/Juxie 1986. [4] G. Chw, and M. 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Salnieron, "Analysis and Sinidation of the instantancons conipnents current in multiphase systems with no linear loads and nonsinusoidal voltages", "Analisis y Simulacibn de las Conipnentcs Instantrineas de Intensidad en Sistenias Polifisicos con Cargas no Lineales y Tensiones no Senoidales", Ph.D. dissertation. Dpt. of Electrical Eiig., E.T.S.I.I., Univ. of Seville, Spain, Noveniber 1993. [ I O ] P. Salmer6q J. C. Montaiio, "Instantaneous Compncnts Current in Polyphascs Systems:, "Componentes Instantineas de Intensidad en Sistenias Polifasicos", IV Jomadas Luso-Espanholas de Enghenaria Electrotemica, Vo1.3, Oporto, Julio, 1995. 1111 S. Fryze, "Effective, Wattelss and Apparent Power in Electrical Circuits for the Case of NoriSinusoidal Wave-Form of Current and Voltage", Elektrotechnische Zeitschri It. Vol. 53, pp. 596-625. 1932. [I21 L. Salazar, G. J&s, "PSPICE Simulation of Three-Pliase Inverters By Means of Switching Functions", IEEE Trans. on Power Electronics, Vo1.9, No.1, January 1994. [I31 P. Salmerbn and J. C. Montatio, "Simulation of instantaneous reactives currents in no linear thee-phases loads", "Siniulacion de las Components Reactivas lnstantancas de Intensidad en Cargas Trifisicas no Linealcs", I11 Jorriadas Hispano Lusas de Ingenieria EICctrica, vol. IV, July 1993. 1141 P. Salmerhn, J.C. Montaiio, "Compensation of no linear thee-pliase loads", "Compensaci6n de cargas trifkicas no lincalcs", Energia, No. 4, lulio/Agosto 1995. 1546