International Journal of Inventions in Reasearch, Engineering Science and Technology (IJIREST),Vol.1,No.1,April 2014 ISSN(Print):2348-7399 ISSN(Online):2348-8077 STUDY AND SIMULATION ANALYSIS OF SINGLE ENDED PRIMARY INDUCTANCE voltage source, aCONVERTER switch, a diode, an inductor, a capacitor and a resistive load. This converter is also Amit Patel 1, Kamal Singh 2, Sandeep Kumar Singh 3 converter because the voltage called the step-down Department of Electrical Engineering across the inductor opposes supply voltage. The circuit Bhagwant Institute of Technology, Muzaffarnagar1,3diagram Radha Govind of buckEngineering converter isCollege, shown inMeerut figure21. amitpatel1287@gmail.com1, kamalsingh32@gmail.com2, san62638@gmail.com3 Abstract: This paper presents study and simulation analysis of Single Ended Primary Inductance Converter (SEPIC) dc-dc converter. The paper introduces the power converters with an overview of different types of basic dc-dc converters. Also brief applications of the dc-dc converters are described. The working of SEPIC converter is explained with advantages and disadvantages. The simulink models of open loop and closed loop for SEPIC converter is designed and simulated. The output voltage and current waveforms without and with using PI controller are obtained. Fig. 1 Circuit diagram of buck converter When switch turns on current flows from the source through switch to inductor L, then capacitor C0 and finally to the resistive load R. As current flows through L, a magnetic field is build up, causing energy to be stored in the inductor. When switch is turned off, energy stored in the inductor supplies current to the resistive load through diode D. The voltage across the load is a fraction of input voltage. This fraction is known as duty cycle (D). Thus the output voltage of buck converter can be varied as the fraction of input voltage by varying the switching duty cycle. The boost converter has similar structure as the buck converter, only the difference is that it has components arranged in different manner. The output of boost is always greater than input voltage therefore the boost converter is used when higher output voltage is required than the input voltage. It is also known as stepup converter because the voltage across inductor L adds to the input supply voltage to step-up the voltage above input voltage. figure 2 shows the circuit diagram of boost converter. Keywords — SEPIC converter, MATLAB Simulink, Dc-dc power conversion, PI controller. I. INTRODUCTION The power converters are the electronic circuits which are used for the conversion, control and conditioning of electric power. The power range may be from mill watts to megawatts as in electro mobile phones and in electric power transmission system simultaneously. Electronic devices and control circuits must be highly robust to achieve a high useful life and the total efficiency of the power electronic circuits must be as high as possible. The most common technology in all the electronic converters is switched mode power converters. Switched mode power converters convert the voltage input to another voltage signal by storing the input energy and them releasing that energy to the output at a different voltage as per switching operation. The most common classification of power conversion systems is based on the waveforms of input and output signals. Thus power converters are classified as ac to dc converters, dc to ac converters, ac to ac converters and dc to dc converters. There are different kinds of dc-dc converters used for several years for different applications. Some of the applications require high voltages while some require low voltages. Depending on the application dc-dc converters are divided as Buck converters, Boost converters, Buck-boost converters, Cuk converters and SEPIC converters. The brief introduction of these dc-dc converters is introduced in this section. In buck converter, the average output voltage is less than the input voltage. Buck converter is made of a Fig. 2 Circuit diagram of boost converter When switch is turned on current flows through inductor L and switch, Thus storing the energy in the inductor in magnetic field. There is no current flowing through diode D and the load current is supplied through the charge stored in capacitor C0. When switch is turned off, the inductor L opposes any drop in current. Thus the inductor voltage adds to the source voltage, thus 35 International Journal of Inventions in Reasearch, Engineering Science and Technology (IJIREST),Vol.1,No.1,April 2014 ISSN(Print):2348-7399 ISSN(Online):2348-8077 was stored in L1. When switch is turned on again, CS discharges through L2 into the load, with L2 and C0 acting as smoothing filter, whereas at the same time energy is being stored in L1. stepping up the output voltage. The current now flows from the source through inductor L, diode D and the load, and then charging the capacitor again. The Buck-boost converter is the combination of buck and boost converter. The components of buckboost converter are similar but arranged in different way to provide step up and step down voltage. The circuit diagram of buck-boost converter is shown below:- II. SEPIC CIRCUIT AND OPERATION Single ended primary inductor converter (SEPIC) is a type of converter that allows the electrical potential i.e. voltage at its output to be greater than or less than to that at its input. The output of the SEPIC converter is controlled by the duty cycle of the switch. The SEPIC converter exchanges energy between the capacitors and inductors in order to convert from one voltage to another. The amount of energy exchanged is controlled by switch S. The energy to increase the current in inductor L1 coming from the input source. The power circuit of the SEPIC converter is presented in figure 5. Fig. 3 Circuit diagram of buck-boost converter When the switch is turned on, there is path between the inductor L and voltage source. As current flows through the inductor L, energy is stored in magnetic field. The diode D is reverse biased so no current flows through the diode D to the load .The capacitor C supplies the load current. When the switch is turned off, the path between the inductor L and voltage source is broken. The stored energy in the inductor L generates a voltage which forward biases the diode D and current flows into load and capacitor causing recharging the capacitor. The buck, boost and buck-boost converters all transfer the energy between input and output using the inductor, thus building the voltage across the inductor where as The cuk converter transfers the energy through the capacitor. The output of cuk converter is inverted and the circuit configuration is the combination of buck and boost converters as in buck-boost converter. figure 4 shows the block diagram of cuk converter. Fig. 5 Circuit diagram of SEPIC converter When the switch is on then switch acts like a short circuit, and the instantaneous voltage across capacitor CS is approximately Vi, the voltage across inductor L2 is approximately –Vi. Therefore, the capacitor CS supplies the energy to increase the magnitude of the current in inductor L2 and thus increase the energy stored in L2. When switch S is turned off, the current in capacitor CS becomes the same as the current in inductor L1, since inductors do not allow instantaneous changes in current. The power is delivered to the load from both L2 and L1. CS, however is being charged by L1 during this off cycle, and will in turn recharge L2 during the on cycle. The ratio between the input and output is D Vo = 1−D (1) Vi III. ADVANTAGES AND DISADVANTAGES OF SEPIC Fig.4 Circuit diagram of cuk converter When the switch is turned on, the path of swich is shorted whereas the diode D0 is open circuited .The current flows through inductor L1 and energy is stored in magnetic field in inductor. When switch is turned off, thus the path across the switch is open circuited. The diode conducts and the current flows from voltage source, through inductor L1, diode D0 and charging capacitor CS by transferring to it some of the energy that The advantages of SEPIC converter are given below: The output voltage can be less than or greater than the input voltage. having non-inverted output i.e. the output voltage is of the same polarity as the input voltage. The output stage rectifier diode is used as a reverse blocking diode. 36 International Journal of Inventions in Reasearch, Engineering Science and Technology (IJIREST),Vol.1,No.1,April 2014 ISSN(Print):2348-7399 ISSN(Online):2348-8077 the isolation between its input and output i.e. provided by a capacitor in series. The disadvantages of SEPIC converter are given below: circuit complexity because two inductors and two capacitors are needed. extra conduction loss in the switch. MULTIPLIER CAPACITOR,CM 660nF OUTPUT CAPACITOR,Co 500μF SWITCHING FREQUENCY,fS 48kHz GRID FREQUENCY,fG 50Hz The values of PI controller parameters are selected by using the trial and error method. PI controller parameters for the SEPIC converter obtained by trial and error method are as follows:Proportional Gain, Kp = 0.2 Integral Gain, Ki = 0.000002 IV. APPLICATIONS OF DC-DC CONVERTERS The different types of applications of the dc-dc converters are given below: Used in high performance dc drive systems like electric traction, electric vehicles and machine tools. Used in radar and ignition systems. Used as photo voltaic arrays, fuel cells or wind turbines. Used in drivers where the breaking of dc motor is desired like transportation system with frequent stops. In the utility ac grid as backup source of energy like battery pack. In uninterrupted power supplies to adjust the level of a rectified grid voltage to that of back up source. In solar systems and in high brightness light emitting diodes. In computer power supplies, battery chargers, dc motor power systems and in different industrial applications. Fig.6 The open loop Simulink model of SEPIC converter V. SIMULATION RESULTS The designed parameters of the SEPIC system is given in table-1. The open loop and closed loop Simulink models for the SEPIC converter is shown in figure 6 and 7. The single phase 115V, 50 Hz ac voltage is the input of the SEPIC. Open loop and closed loop output voltage and current waveforms of SEPIC are shown in figures from 8 to 15 respectively. Different parameters of the SEPIC are given table-1. Table-1: Parameters of the SEPIC. MODEL PARAMETERS VALUES INPUT VOLTAGE,Vi 115V OUTPUT VOLTAGE,Vo 345V INDUCTOR,L1 1mH INDUCTOR,L2 500μH SERIES CAPACITOR,CS 660nF Fig.7 The closed loop Simulink model of SEPIC converter 37 International Journal of Inventions in Reasearch, Engineering Science and Technology (IJIREST),Vol.1,No.1,April 2014 ISSN(Print):2348-7399 ISSN(Online):2348-8077 Fig.12 Output voltage waveform of closed loop SEPIC converter with Vref =700V Fig.8 Output voltage waveform of open loop SEPIC converter Fig.13 Output current waveform of closed loop SEPIC converter with Vref =700V Fig.9 Output current waveform of open loop SEPIC converter Fig.14 Output voltage waveform of closed loop SEPIC converter with Vref =200V Fig.10 Output voltage waveform of closed loop SEPIC converter with Vref =345V Fig.15 Output current waveform of closed loop SEPIC converter with Vref =200V Fig.11 Output current waveform of closed loop SEPIC converter with Vref =345V 38 International Journal of Inventions in Reasearch, Engineering Science and Technology (IJIREST),Vol.1,No.1,April 2014 ISSN(Print):2348-7399 ISSN(Online):2348-8077 V. CONCLUSIONS [8] The SEPIC converter is designed and simulated. The converter model is simulated on Simulink for open loop as well as closed loop. The PI controller is used to control the output voltage of the SEPIC which gives the controlled variation of output voltage. The output voltage varies from 200V to 700V efficiently with the help of PI controller. The closed loop waveforms show that the rise time and peak time of the output signals are less than that the output waveforms of open loop system. Thus SEPIC converter works as a good dc-dc converter with high output voltage variation. 2003. REFERENCES [1] [2] [3] [4] [5] [6] [7] Power Electron., vol. 23, no. 2, pp. 871–887, Mar.2008. Q. Zhao and F. C. Lee, “High-efficiency, high step-upDC–DC converters,” IEEE Trans. Power Electron., vol. 18, no. 1, pp. 65–73, Jan. P. F. de Melo, R. Gules, R. Romaneli, and R. C. Annunziato, “A Modified SEPIC Converter for High-Power-Factor Rectifier and Universal Input Voltage Applications IEEE Trans.Power Electron., vol. 25, no. 2, pp. 310–321, Feb. 2010. J. Chen, D. Maksimovic, and R. W. Erickson, “Analysis and design of a low-stress buckboost converter in universal-input PFC applications,”IEEE Trans. Power Electron., vol. 21, no. 2, pp. 320–329, Mar. 2006. J. Qian and F. C. Lee, “A high efficient single stage single switch high power factor ac/dc converter with universal input,” IEEE Trans. Power Electron., vol. 13, no. 4, pp. 699–705, Jul. 1998. C. Qiao and K. M. Smedley, “A topology survey of single-stage power factor corrector with a boost type input current-shaper,” IEEE Trans. Power Electron., vol. 16, no. 3, pp. 360– 368, May 2001. M. H. L. Chow, Y. S. Lee, and C. K. Tse, “Single-stage single-switch isolated PFC regulator with unity power factor, fast transient response, and low-voltage stress,” IEEE Trans. Power Electron., vol. 15, no. 1,pp. 156–163, Jan. 2000. J. L. Lin, W. K. Yao, and S. P. Yang, “Analysis and design for a novel single-stage high power factor correction diagonal halfbridge forward ac-dc converter,” IEEE Trans. Power Electron., vol. 53, no. 10, pp. 2274– 2286, Oct. 2006. M. Prudente, L. L. Pfitscher, G. Emmendoerfer, E. F. R. Romaneli, and R. Gules, “Voltage multiplier cells applied to nonisolated DC–DC converters,”IEEE Trans. 39