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Ideal Institute of Technology, Ghaziabad Electronics & communication Engineering Department SVPWM CONTROLLED INVERTER FOR POWER CODITIONING Muneer Ahamed Khan (Assistant Professor) INTRODUCTION 1.1 The growing use of non-linear and time-varying loads has led to distortion of voltage and current waveforms and increased reactive power demand in ac mains. Harmonic distortion is known to be source of several problems, such as increased power losses, excessive heating in rotating machinery, and harmonic resonances in the utility, significant interference with communication circuits, flicker and audible noise, incorrect operation of sensitive loads [1,2]. Traditionally, LC tuned passive filters have been used to absorb harmonic currents generated by nonlinear loads. Their main advantage is high reliability and low cost. However, passive filters have several drawbacks, which may cause harmonic interaction with the utility problems with the utility system, in the presence of stiff utility sharp tuning of the LC filter is required and may not meet the specified harmonic current limits [3, 4]. This provides the motivation for investigation of an active filter topology, which is practically viable, cost effective and can meet the recommended standard for high power nonlinear loads. For high-power applications, the active filters are not cost effective due to their large rating and high switching-frequency requirement of the Pulse Width Modulation (PWM) inverter. 1.2 PWM TECHNIQUE Because of advances in solid state power devices and microprocessors, switching power converters are used in industrial application to convert and deliver their required energy to the motor or load. PWM signals are pulse trains with fixed frequency and magnitude and variable pulse width. There is one pulse of fixed magnitude in every PWM period. However, the width of the pulses changes from pulse to pulse according to a modulating signal. When a PWM signal is applied to the gate of a power transistor, it causes the turn on and turns off intervals of the transistor to change from one PWM period to another PWM period according to the same modulating signal. The frequency of a PWM signal must be much higher than that of the modulating signal, the fundamental frequency, such that the energy delivered to the motor and its load depends mostly on the modulating signal. The advantage of PWM based switching power converter over linear power amplifier is: 1 Lower power dissipation 2 Easy to implement and control 3 No temperature variation and aging-caused drifting or degradation in linearity 4 Compatible with today’s digital micro-processors Fig. 1.1 Symmetric and Asymmetric PWM Signals Fig 1.1 shows two types of PWM signals, symmetric and asymmetric. The pulses of a symmetric PWM signal are always symmetric with respect to the center of each PWM period. The pulses of an asymmetric PWM signal always have the same side aligned with one end of each PWM period. It has been shown that symmetric PWM signals generate fewer harmonics in the output currents and voltages. This literature is considers three popular PWM techniques for the mostly used three phase voltage source power inverter applications. This is the most popular method of controlling the output voltage and this method is termed as Pulse-Width Modulation (PWM) Control. The advantages possessed by PWM techniques are as under: The output voltage control with this method can be obtained without any additional components. With this method, lower order harmonics can be eliminated or minimized along with its output voltage control. As higher order harmonics can be filtered easily, the filtering requirements are minimized. The main disadvantage of this method is that SCRs are expensive as they must possess low turnon and turn-off times. PWM techniques are characterized by constant amplitude pulses. The width of these pulses is however modulated to obtain output voltage control and to reduce its harmonic content. The different PWM techniques are as under: a) Single-pulse modulation b) Multiple pulse modulations c) Sinusoidal pulse width modulation (Carrier based Pulse Width Modulation Technique) 1.3 SVPWM TECHNIQUE SVPWM technique was originally developed as a vector approach to pulse width modulation for three-phase inverters. The SVPWM method is frequently used in vector controlled applications. In vector controlled applications this technique is used for reference voltage generation when current control is exercised. It is a more sophisticated, advanced, computation intensive technique for generating sine wave that provides a higher voltage with lower total harmonic distortion and is possibly the best among all the pulse width modulation techniques. It confines space vectors to be applied according to the region where the output voltage vector is located. Because of its superior performance characteristics, it is been finding wide spread applications in recent years. The main aim of any modulation technique is to obtain variable output voltage having a maximum fundamental component with minimum harmonics. Many PWM techniques have been developed for letting the inverters to posses various desired output characteristics to achieve the wide linear modulation range, less switching losses, lower harmonic distortion. The SVPWM technique is more popular than conventional technique because of its excellent features. More efficient use of DC supply voltage 15% more output voltage then conventional modulation Lower Total Harmonic Distortion (THD) Prevent un-necessary switching hence less commutation losses 1.4 PRINCIPLE OF SVPWM Firstly model of a three-phase inverter is presented on the basis of space vector representation. The threephase VSI is reproduced in Fig. 1.2. S1, to S 6, are the six power switches that shape the output, which are , , controlled by the switching variables a, a , b , b , c and c , When an upper transistor is switched on, i.e., , , , the corresponding a , b , , or c is 0 . Therefore, the on and off states of the upper switches S1, S3, S5, can be used to determine the output voltage. + S1 a Vdc C + S5 c Va - Vab Vb a’ S4 - S3 b b’ S6 Vc c’ S2 Vca N Vbc Load Fig. 1.2 Power circuit of a three-phase VSI The relationship between the switching variable vector [a b c ]t and line-to-line voltage vector [ Vab, Vbc, Vca ] is given by (5.6) in the following: Vab 1 1 0 a V V 0 1 1 b dc bc Vca 1 0 1 c (1.1) Also, the relationship between the switching variable voltage vectors [ Vab, Vbc, Vca ]t can be expressed below. Van V Vdc bn 3 Vcn 2 1 1 a 1 2 1 b 1 1 2 c (1.2) .One simple method of approximation is to generate the one simple method of approximation is to generate the average output of the inverter in a small period, T to be the same as that of V ref in the same period. . The angle of the reference voltage is hold for each switching period so that its value does not change during time calculation. A ramping time signal is generated using repeating sequence block. CHAPTER 2 Simulink Model : In following figure different simulink model using PWM & SVPWM technique have been discussed . Their result have been compared also. Fig. 2.1Simulink model of PWM technique for nonlinear load condition with APF Fig 2.2Source current waveform with PWM technique for nonlinear load condition with APF 0 -10 0 0.2 0.4 0.6 0.8 1 Time (s) Mag (% of Fundamental) Fundamental (50Hz) = 8.793 , THD= 13.26% 30 25 20 15 10 5 0 0 5 10 Harmonic order 15 20 SVPWM technique for nonlinear load (rectifier with R load) condition with APF Fig. 2.3 Simulink model of SVPWM technique for nonlinear load condition with APF Selected signal: 50 cycles. FFT window (in red): 2 cycles 10 0 -10 Fig. 2.4 Source Current waveform with SVPWM technique for nonlinear load condition with APF 0 0.2 0.4 0.6 0.8 1 Time (s) Fundamental (50Hz) = 6.964 , THD= 5.47% Mag (% of Fundamental) 4 3 2 1 0 0 5 10 Harmonic order 15 Fig. 2.5 Harmonic spectrum of SPWM technique for nonlinear load condition with APF 20 SVPWM technique for nonlinear load (rectifier with R load) condition with APF Fig. 2.8Simulink model of SVPWM technique for nonlinear load condition with APF Fig. 2.9 Source Current waveform with SVPWM technique for nonlinear load condition with APF 0 -10 0 0.2 0.4 0.6 0.8 1 Time (s) Fundamental (50Hz) = 6.964 , THD= 5.47% Mag (% of Fundamental) 4 3 2 1 0 0 5 10 Harmonic order 15 20 Fig. 2.10 Harmonic spectrum of SPWM technique for nonlinear load condition with APF 1.7 SIMULATION RESULT ANALYSIS AND DISCUSSIONS From the simulated results of different cases without and with active filter are shown in following tables. Table1.1 Result Analyses for non linear System. Without APF THD Source Site PF 30.28% 0.92 Non Linear Load PWM Technique with APF THD Source Site PF 13.26% 0.94 SVPWM technique with APF THD Source Site PF 5.47% 0.95 From Table 1.1 show the simulation of harmonic spectrum of linear three phase balance and unbalance load. is shown in fig harmonic spectrum of the current before compensation on the load side. The source current total harmonic distortion (THD) is 0.00%. It should be noted that no harmonic generated in linear three phase balance system. From Table 1.1 shows the simulation of harmonic spectrum of linear three phase unbalance load. is the harmonic spectrum of the source current before compensation on the source side. The source current total harmonic distortion (THD) is 0.00%. It should be noted that no harmonic generated in linear three phase unbalance system. From aboveTable shows the simulation of harmonic spectrum of APF with PWM Technique and SVPWM Technique used for non linear load used when the non-linear is a three-phase diode bridge rectifier with resistance-inductive load. is the harmonic spectrum of the source current before compensation on the source side. The harmonic spectrum of the source current shows that magnitude of the 5th, 7th, 11th and 13th harmonics are evidently reduced after compensation. The source current Total Harmonic Distortion (THD) is 30.21%, before compensation and after compensation the supply current THD is 13.26% when PWM Technique used this is shown by Fig. . When the SVPWM technique used the supply current Total Harmonic Distortion (THD) is 5.47%, this is shown by Fig. It should be noted that the higher frequency harmonics caused by APF in mains current can be canceled easily by a small passive filter and there are pulses in main current at the points, where di dt of load current is large, because fixed switching frequency restrict the tracking capability of APFfrom the above results the performance of balanced linear load, unbalanced linear load and non linear load with the proposed control algorithm is observed. The three-phase source voltage is made in phase with source current for balanced linear load. The three-phase source current is made equal in magnitude when an unbalanced linear load is simulated. The harmonic spectrum shows that reduction of higher order harmonics in three-phase source current when non-linear load is simulated. References 1) EI-Habrouk. M, Darwish. M. K, Mehta. P, “Active power filters-A review,” Proc IEEE Elec. Power App., Vol. 147, No. 5 , pp. 403-413, September 2000. 2) Akagi H., “New trends in active filters for power conditioning,” IEEE Trans. on Ind. app, Vol. 32, No. 6, pp. 1312-1322 , November-December, 1996. 3) Singh. B, Al-Haddad. K and Chandra. A, “Review of active filters for power quality improvement,” IEEE Trans. Ind. Electron., Vol. 46, No. 5, pp. 960-971, October, 1999. 4) Rathnakumar. D, Lakshmana Perumal, Srinivasan. T, “A new software implementation of space vector PWM,” IEEE Trans. Power Electron., Vol.14, pp.131-136, 8-10 April, 2005. 5) Atif Iqbal, Lamine. A, Imtiaz Ashraf, and Mohibullah, “MATLAB model of Space Vector PWM for three-phase voltage source inverter,” Universities Power Engineering Conf. 2006, UPEC’06, proceedings of the 41st international Vol. 3, pp.1096-1100, 6-8 September, 2006. 6) Wang Jianze, Peng Fenghua, Wu Quitao, and Ji Yanchao, “A novel control method for shunt active power filters using SVPWM,” IEEE Trans. on Ind. app., Vol.1, pp.134-139, 3-7 October, 2004. 7) Dan.S.G, Benjamin.D.D, Magureanu.R, Asimionoaei.L, Teodorescu.R, and Blaabjerg. F, “Control strategies of active filters in the context of power conditioning,” IEEE Trans. on Ind. App., Vol. 25, pp.10-20, 11-14 September, 2005 8) T. Mahalekshmi “Current Harmonic Compensation and Power Factor Improvement by Hybrid Shunt Active Power Filter” Int. J. of Computer Applications (0975 – 8887), Vol. 4, No.3, July, 2010. 9) Luis A. Morán, Juan W. Dixon, Jose R. Espinoza and Rogel R. Wallace “Using active power filters to improve power quality”. 10) António P. Martins “The Use of an Active Power Filter for Harmonic Elimination and Power Quality Improvement in a Nonlinear Loaded Electrical Installation”. 11) Emílio F. Couto, Julio S. Martins, and Joao L. Afonso “Simulation Results of a Shunt Active Power Filter with Control Based on p-q Theory”.