Shunt Active Power Filter for Compensation of System Harmonics

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Volume 5, Issue 1 (February, 018) E-ISSN : 48-7 P-ISSN : 454-1 Shunt Active Power Filter for of System Harmonics Badal Devanand Umare 1, A. S. Sindekar 1 PG Scholar, HOD, Department of Electrical Engineering, Govt. College of Engineering, Amravati, India 1 badal.umare10@gmail.com, assindekar@rediffmail.com Abstract: The abundant use of power electronics based equipment/systems have produced an important impact on the power quality of electric power supply distribution system. The non-linear type domestic and industrial loads injects harmonics in the system voltages. Besides, many of the equipment causing the harmonic distortions are sensitive to the deviations from the ideal sinusoidal line voltage. Shunt active power s are well known to compensate the system harmonics. This paper presents the classification of active s, simulation of shunt active power based on p-q theory control strategy and results in the form of waveform of source current before compensation and after compensation have been shown. Keywords: Shunt Active Harmonic Power Filter, Harmonics, Non-Linear Load, P-Q Theory, PWM Inverter, FFT Analysis. I. INTRODUCTION With significant development of power electronics technology, the increase of nonlinear loads such as static power converters has decreased power quality in power transmission and distribution systems. Notably, voltage harmonics resulting from current harmonics produced by the nonlinear loads have become a serious problem in many countries. Harmonics in power systems have been suppressed so far by shunt passive s. However, shunt passive s have many problems to discourage their applications. As shown in Fig. 1, a shunt passive exhibits lower impedance at a tuned harmonic frequency than the source impedance to reduce the harmonic currents flowing into the source. The impedance ratio of the source decides the ing characteristics of the shunt passive. Therefore the shunt passive has the following problems. i) The source impedance, which is not accurately known and varies with the system configuration strongly influences ing characteristics of the shunt passive. ii) The shunt passive acts as a current sink to the harmonic voltage included in the source voltage V S. In the worst case, shunt passive falls in series resonance with the source impedance []. To cope up with these demerits of shunt passive continuous efforts have been put by power electronics researchers on development and design of shunt active power [7]. In shunt active power, the harmonic component and reactive power required by the non-linear load is fed separately so that the source has to supply only sinusoidal component. In other words, harmonic current component being fed by shunt active power into the line is 180 degree phase opposition to the harmonic component drawn by non-linear load and they get cancel out [8]. The general schematic of shunt active power is shown in Fig.. Fig. General Schematic of Shunt Active Power Filter In this paper simulation of shunt active power incorporating control topology based on reactive power p-q theory is presented.the shunt active power considered here satisfactorily compensates the harmonic contents of source current. II. CLASSIFICATION OF ACTIVE FILTER Fig. 1 Basic Principle of Shunt Passive Filter In many technical literatures, various types of active s have been proposed. The classification of active s is done in many ways. Active s are classified mainly in two types, ac and dc s. Active dc s have been designed to compensate for current and/or voltage harmonics on the dc side of thyristor converters for HVDC systems and on the dc link of a PWM rectifier/inverter for traction systems. The term active s refers to active ac s in most cases. 16

Volume 5, Issue 1 (February, 018) E-ISSN : 48-7 P-ISSN : 454-1 A. Classification by Objectives: Who Is Responsible for Installing Active Filters? The objective of who is responsible for installing active s classifies them into the following two groups: Active s installed by individual consumers on their own premises near one or more identified harmonic producing loads Active s installed by electric power utilities in substations and/or on distribution feeders. The main purpose of the active s installed by individual is to compensate current harmonics and current imbalance of their own harmonic producing loads. On the other hand, the primary purpose of active s in the near future will be to compensate voltage harmonics and voltage imbalance, or to provide harmonic damping throughout power distribution systems. In addition, active s have the function of harmonic isolation at the utility consumer point of common coupling in power distribution systems. B. Classification by System Configuration : 1) Shunt Active Filters and Series Active Filters A system configuration of a shunt active when it is used alone is shown in Fig. 4, which is one of the most fundamental system configurations. The shunt active is controlled to draw a compensating current, I AF from the utility, so that it cancel current harmonics on the ac side of a general purpose diode rectifier with a dc link inductor [4] or a PWM rectifier with a dc link capacitor for traction systems [6]. The shunt active has the capability of damping harmonic resonance between an existing passive and the supply impedance []. A system configuration of a series active used alone is shown in Fig. 5. The series active is connected in series with the utility through a matching transformer, so that it is applicable to harmonic compensation of a large capacity diode rectifier with a dc link capacitor. Table I shows comparison between the shunt and series active s. Fig. 5 Series Active Filter Used Alone Table I. Comparision of Shunt And Series Active Filter Used Alone System Configuration Power Circuit Of Active Filter Active acts as Additional Function Present Situation Shunt Active Filter Series Active Filter Figure 4 Figure 5 Voltage Fed PWM Inverter with Current Minor Loop Current source: I AF Reactive Power Commercial Stage ) Hybrid Active/Passive Filters: Voltage Fed PWM Inverter without Current Minor Loop Voltage source: V AF Ac Voltage Regulation Laboratory Level Three types of hybrid active/passive s are shown in Figs. 6-8. To reduce initial cost and to improve efficiency are the main purpose of these hybrid active/passive s. The shunt passive consists of one or more tuned LC s and/or a high-pass. Table II shows comparison among three hybrid s, in which the active s are different in function than the passive s. The combination of shunt active and passive s have already been applied to harmonic compensation of large rated cycloconverters for steel mill drives []. The combined s (shown in Fig. 4 and in Fig. 5) will be practically applied in the near future, not only for harmonic compensation but also for harmonic isolation between supply and load, and for voltage regulation and imbalance compensation. They are considered prospective alternatives to shunt or series active s used alone. Comparison of Shunt active plus shunt passive, Series active plus shunt passive and Series active connected in series with shunt passive is shown in Table II. Fig. 4 Shunt Active Filter Used Alone 164

Volume 5, Issue 1 (February, 018) E-ISSN : 48-7 P-ISSN : 454-1 Fig. 6. Combination of Shunt Active Filter and Shunt Passive Filter Fig. 7. Combination of Shunt Passive Filter and Series Active Filter Problems or issues Present situation Share compensation in frequency domain between active and passive Commercial stage active Difficult to protect active against overcurrent and no reactive power control Field testing C. Classification by Power Circuit : No reactive power control Coming in market There are two types of power circuits used for active s: a voltage-fed PWM inverter [] and a currentfed PWM inverter [1]. These are similar to the power circuits used for ac motor drives. They are, however, different in their behavior because active s act as non-sinusoidal current or voltage sources. The voltagefed is preferred to the current-fed PWM inverter because the voltage-fed PWM inverter is higher in efficiency and lower in initial cost than the current-fed PWM inverter [5]. III. INSTANTANEOUS REACTIVE POWER P-Q THEORY In this paper p-q theory is presented for determining the compensation current need to be injected into the network at the Point of Common Coupling (PCC) feeding non-linear loads. Fig. 8. Active Filter Connected in Series with Shunt Passive Filter System configuratio n Function of active Advantage 165 Shunt active plus shunt passive Table II. Series active plus shunt passive Series active connected in series with shunt passive Figure 6 Figure 7 Figure 8 Harmonic compensation or harmonic damping Reactive power controllable Harmonic isolation and harmonic damping No harmonic current flowing through Harmonic compensatio n or harmonic damping Easy protection of active It involves an algebraic transformation of three -phase power system voltages and currents in a-b-c coordinates to α-β coordinates. In a-b-c coordinates, the a, b and c axis are fixed on the same plane, apart from each other by π /. Fig. 9. Clarke Transformation In the Clark transformation, three phase system is converted into two phase stationary frame of reference system. From this transformation the voltage and current parameters can be expressed as the sum of two self-dependent vectors which are orthogonal to each other. The instantaneous values of system voltage and current in α-β coordinates is as follows.

Volume 5, Issue 1 (February, 018) E-ISSN : 48-7 P-ISSN : 454-1 v α v β Where, A A = = A v a v b v c and i α i β = Transformation matrix 1 1 0 1 = A i a i b ic (1) V(t) = V α (t)i +V β (t)j () I(t) = I α (t)i + I β (t)j () The active power is the dot product of voltage and current whereas reactive power is the cross product of voltage and current p(t) = V(t).I(t) (4) q(t) = V(t) I(t) (5) p(t) = V α (t)i α (t) +V β (t)i β (t) (6) q(t) = V α (t)i β (t) V β (t)i α (t) (7) p(t) and q(t) are divided into two parts namely average part which is non-oscillating whereas the other part is oscillating. p(t)=p(t)+p (t) (8) q(t)=q(t)+q (t) (9) Since component P (t) does not involve in any energy transfer from supply to load, it must be compensated. Similarly q(t) which is reactive power it also does not involve in any energy transfer from supply to load it also must be compensated. We have to also compensate switching losses of the inverter which is known as P loss. Now Referring P (t) +P loss and q(t), the reference current can be generated which decides the switching state of inverter. The reference current of the shunt active power must include the values of P (t), P loss, Q(t) and Q (t). In this case, the reference currents required by the shunt active power are calculated as follows i cα i cβ = 1 v α +v β v α v β v β v. P (t) + P loss α Q t + Q (t) (10) Now, this is in α-β co-ordinate but we need reference compensation current in a-b-c co-ordinate, by taking inverse clarke transformation we get, i ac i bc i cc Where, A = = A i cα i cβ (11) 1 0 1 1 IV. SIMULATION OF SHUNT ACTIVE POW ER A. Simulation Model: FILTER The simulation model with and without Shunt Active Power Filter has been developed based on P-Q theory for harmonic compensation as Shown in Fig. 10. The various subsystems of the active harmonic power circuit configuration have been simulated and the gate drive signals for the switching devices have been 166 Fig. 10. Simulation Model of Shunt Active Power Filter appropriately generated for the Pulse Width Modulation (PWM) inverter. B. Simulation Results:

Volume 5, Issue 1 (February, 018) E-ISSN : 48-7 P-ISSN : 454-1 The topology of active harmonic discussed in the previous section has been investigated and subsequently validated through simulation software and the results (waveforms) obtained are shown in Fig. 11 and Fig. 1 for an electrical network, in which source current before compensation and after the compensation have been plotted. Fig. 14 FFT Analysis after Harmonic Current Fig. 11. Source Current before Harmonic Current The three phase six pulse bridge rectifier with resistive load is considered as a nonlinear load connected to the feeder line giving the Total Harmonic Distortion (THD) of.6% as shown in Fig. 1. The dominant harmonics in this system are 5 th and 7 th (as per np±1 where n is integer and p is number of pulses). The waveform of source current after harmonic current compensation is shown in Fig. 1. The reference current should contain all these harmonics for the requirement of actual compensation in out of phase manner. Thus, the Total Harmonics Distortion (THD) obtained after the compensation is found reduced to 0.6%. V. CONCLUSION Simulation model of shunt active power has been simu lated with the help of control topology based on p- q theory for three phase system and results are found satisfactory. On the basis of results obtained it is concluded that the harmonic level of the system is reduced from.6% to 0.6% after application of shunt active power, meeting IEEE: 519 guidelines. VI. REFERENCE [1] H. Kawahira, T. Nakamura, S. Nakazawa, and M. Nomura, Active power s, in Proc. 198 Int. Power Electronics Conf, To kyo. JaDan. pp. 981-99, 198. [] M. Takeda, K. Ikeda, and Y. Tominaga, Harmonic current compensation with active, in Proc. 1987 IEEE/IAS Annual Meeting, pp. 808-81s, 1987. Fig. 1. FFT Analysis before Harmonic Current [] Fang Zheng Peng, H. Akagi, A. Nabae, A New Approach to Harmonic in Power Systems-A Combined System of Shunt Passive and Series Active Filter, IEEE transactions on industry applications. vol. 6. no. 6. November /December 1990. [4] H. Akagi, Y. Tsukamoto, and A. Nabae, Analysis and design of an active power using quadseries voltage-source PWM converters, IEEE Transactions Industrial Application., vol. 6, pp. 9-98, 1990. [5] H. Akagi, Trends in active power line conditioners, IEEE Trans. Power Electronics, vol. 9, pp. 6-68, 1994. Fig. 1. Source Current after Harmonic Current 167 [6] J. 0. Krah and J. Holtz, Total compensation of lineside switching harmonics in converter-fed ac

Volume 5, Issue 1 (February, 018) E-ISSN : 48-7 P-ISSN : 454-1 locomotives, in Proc. IEEE/IAS Annual Meeting, pp. 91-90, 1994. [7] Les zek S. Czarnecki, Instantaneous Reactive Power p-q Theory and Power Properties of Three- Phase Systems, IEEE Trans. Power Delivery, vol.1, no.1, pp.6-67, Jan 006. [8] Gaurava Deep Srivastava, Rajendrakumar D. Kulkarni Design, Simulation and Analysis of Shunt Active Power Filter using Instantaneous Reactive Power International Conference on Nascent Technologies in the Engineering Field (ICNTE- 017), 017. 168