ISSN 2394-3777 (Print) ISSN 2394-3785 (Online) Available online at www.ijartet.com International Journal of Advanced Research Trends in Engineering and Technology (IJARTET) Vol. II, Special Issue XIII, March 2015 Modified Bridgeless Resonant Converter with Power Factor Correction for LED Applications V. Velmurugan1, Dr.A. Gnanasaravanan2, R. Arul Jose3 PG Scholar, Power Electronics and Drives, SCAD College of Engineering and Technology, Tirunelveli, India 1 Professor, SCAD College of Engineering and Technology, Tirunelveli, India 2 Assistant professor, SCAD College of Engineering and Technology, Tirunelveli, India 3 Abstract: In the past decade, there is growing awareness about line pollution and deteriorating power factor due to all pervading inductive and non-linear loads. In many real time applications, the conventional diode rectifiers are used to provide a DC supply. The diode rectifiers are non linear in nature and consequently generate harmonic currents in AC line power resulting in low power factor and high percentage total harmonic distortion (THD). The harmonic distortion has several detrimental effects including poor power factor, low percentage efficiency and interfere with the communication, control circuits nearby. This project proposes a novel single-stage Light-Emitting Diode (LED) driver for street-lighting applications with power-factor-corrections. The presented driver integrates a modified bridgeless power-factor-correction (PFC) AC-DC converter with a half-bridge-type LLC DC-DC resonant converter into a single-stage conversion circuit topology. The proposed AC-DC resonant driver provides input current shaping, and it offers attributes of lowered switching losses to the soft-switching functions obtained on two power switches and two output-rectifier diodes. The proposed driver features cost-effectiveness, high circuit efficiency, high power factor and low input current total-harmonics-distortion THD. I. INTRODUCTION Light emitting diodes (LEDs) have favourable features of smaller size, longer lifetime, lower maintenance costs, greater strength against breakage, and being mercury free and therefore less harmful to our environment than traditional lighting sources. Thus, LEDs have become increasingly common in our daily lives. They are well suited to indoor and outdoor energy saving lighting applications, such as traffic lighting, background lighting, displays, street lighting, automotive automotive and motorcycle lighting, decorative lighting, and so on. The installation of street lights is closely related to the development of one area or region, and they represent the financial success of a city. For street lighting applications, the traditional lighting sources are high intensity discharge (HID) high striking voltage for starting the lamp up and an extra high ignition voltage in the hot restart status, and that they offer a long lifetime in comparison to their traditional counterparts. Table I shows some comparisons between traditional and new lighting sources for street-lighting applications. The traditional lighting source is a high pressure sodium lamp (such as a 150W OSRAM NAV-E lamp), and the new one is an LED lamp (a 144W AcBel LM9003-003 G/GT lamp for example) as an alternative option for street lighting circumstances. The LED lamp consumes less power and has better color rendering index and longer lamp life than the traditional one. Instead of traditional HID lighting sources such as high pressure sodium lamps and high pressure mercury lamps, LED, which offers features of satisfying lighting efficiency, reduced power consumption, and long lifetime, will play an important role for streetlight applications in the future. II. A BRIDGELESS POWER FACTOR CORRECTION Lamps, such as high-pressure sodium lamps and CONVERTER USING LLC RESONANCE CONVERTER high- pressure mercury lamps. Recently, LEDs are commonly being used as new sources for street lighting The proposed driver for powering an LED street-lighting applications due to their attractive characteristics of good module with a rated LED power of larger than 70 W is color rendering index (CRI), energy savings, being mercury presented. It combines a modified bridgeless PFC AC-DC free, quickly turning on and off, that they do not require a All Rights Reserved © 2015 IJARTET 8 ISSN 2394-3777 (Print) ISSN 2394-3785 (Online) Available online at www.ijartet.com International Journal of Advanced Research Trends in Engineering and Technology (IJARTET) Vol. II, Special Issue XIII, March 2015 converter with a half-bridge-type LLC DC-DC resonant converter into a single stage of power conversion. Fig.2. The simplified single-stage operational modes. Mode 1: The input utility-line voltage VAC is defined as When vds1 decreases to zero at time instant t0, this mode begins. The power switch S1 turns on with zerovoltage switching (ZVS). The utility-line voltage VAC charges the inductor Lb through the diode D1. The inductor The single-stage driver consists of a filter inductor Lf, a current i linearly increases, and it is given by: Lb filter capacitor Cf, an inductor Lb, two diodes D1 and D2, two power switches S1 and S2, a DC-linked capacitor CB, a resonant capacitor Cr, an inductor Lr, a centre-tapped transformer T1 with two output windings, two diodes D3 and D4 and a capacitor Co, along with the LED street-lighting module. Fig. 4.2 also shows the block diagram for controlling the single-stage LED driver, and the presented control circuit is shown in, a constant-voltage and constantcurrent (CV-CC) controller (IC1 SEA05) is adopted to sense the output voltage through resistors Rvs1 and Rvs2, while simultaneously sensing the output current through the Fig.3. Mode 1 resistor Rcs for supplying the rated voltage and current to The inductors Lm and Lr provide energy to Cr and the experimental LED street-lighting module. The output C through the body diode of S1, and to capacitor Co along signal of the CV-CC controller feeds into the high-voltage B with the LED street-lighting module through diode D3. At resonant controller (IC3 L6599) through a photo-coupler time instant t1, the inductor current iLr becomes zero. In (IC2 PC817). Two gate-driving signals vgs1 and vgs2 addition, the DC-linked capacitor CB provides energy to Cr generating from the resonant controller regulate the output and Lr through the switch S1, and the magnetic inductor Lm voltage and current of the LED street-lighting module by provides energy to the capacitor Co along with the LED utilizing variable-frequency control scheme. Moreover, the street-lighting module through diode D3. At time instant t2, inductor Lb is designed to be operated at discontinuousthe inductor current iLm increases to zero. Moreover, the DCconduction mode (DCM) for naturally achieving power linked capacitor CB provides energy to Cr, Lr and Lm through factor corrections. the switch S1, and to the capacitor Co along with the LED street-lighting module through diode D3. When iD3 decreases III. MODES OF OPERATION to zero, Mode 1 ends. Fig. 5.1 presents the simplified single-stage LED Mode 2: driver for supplying the street-lighting module used to At t3, the utility-line voltage vAC still charges the analyze the operational modes for the positive utility-line inductor Lb through the diode D1. Current iLb reaches its half cycle (the analysis for the negative one is similar). maximum values iLb-pk(t), and can be respectively expressed as Fig.1. LLC DC-DC Converter All Rights Reserved © 2015 IJARTET 9 ISSN 2394-3777 (Print) ISSN 2394-3785 (Online) Available online at www.ijartet.com International Journal of Advanced Research Trends in Engineering and Technology (IJARTET) Vol. II, Special Issue XIII, March 2015 Where TS and D are the switching period and duty cycle of two power switches, respectively. Fig.4. Mode 2 The DC-linked capacitor CB provides energy to Cr, Lr and Lm through the switch S1. The capacitor Co supplies energy to the LED street-lighting module. When iLM is equal to iLr, Mode 2 ends. Mode 3 The utility-line voltage vAC and the inductor Lb provide energy to the capacitor CB through the diode D1, and iLb starts to linearly decrease at t4. The DC-linked capacitor CB along with the intrinsic capacitor CS2 provides energy to Cr, Lr and Lm. The capacitor Co still supplies energy to the LED street-lighting module. When vds2 decreases to zero at t5, Mode 3 ends. The magnetic inductor Lm provides energy to Cr and Lr through the body diode of S2, and to capacitor Co along with the LED street-lighting module through diode D4. When S2 turns on, Mode 4 ends. Mode 5 While S2 is on at t6, Mode 5 begins. The inductor Lb still provides energy to the capacitor CB through the diode D5, and iLb linearly decreases. The inductor Lr provides energy to Cr through the switch S2, and the magnetic inductor Lm provides energy to capacitor Co along with the LED street-lighting module through diode D4. When iLb decreases to zero, Mode 5 ends Fig.7. Mode 5 Mode 6 At t7, the inductor current iLb is zero. The inductor Lr still provides energy to Cr through the switch S2, and the magnetic inductor Lm still provides energy to capacitor Co along with the LED street- lighting module through diode D4. When iLm decreases to zero, Mode 6 ends. Fig.5. Mode 3 Mode 4 At t5, the inductor Lb provides energy to the capacitor CB through the diode D5, and iLb linearly decreases with a down slope of (vAC(t)-VDC)/Lb. The inductor current iLb is given by Fig.8. Mode 6 Mode 7 The inductor Lr still provides energy to Cr and Lm through the switch S2, and to capacitor Co along with the LED street-lighting module through diode D4 during Mode 7. When iD4 decreases to zero, Mode 7 ends. Fig.6. Mode 4 All Rights Reserved © 2015 IJARTET 10 ISSN 2394-3777 (Print) ISSN 2394-3785 (Online) Available online at www.ijartet.com International Journal of Advanced Research Trends in Engineering and Technology (IJARTET) Vol. II, Special Issue XIII, March 2015 Operational Modes 1 to 9 perform in the positive half-cycle of input utility-line voltage, while Modes 10 to 18 occurs in the negative half-cycle. IV. DESIGN OF CONVERTER This section presents a design procedure for the proposed LED street- lighting driver, and a 144W-rated LED streetlighting module with 36V/4A output has been selected as a design example. The design specifications are listed as follows. Fig.9. Mode 7 Mode 8 At t9, the capacitor Cr provides energy to Lr and Lm 1) Input utility-line voltage (rms value): Vac-rms = 100V (Vacthrough the switch S2, and the capacitor Co provides energy MIN) ~120V (Vac-MAX). to the LED street-lighting module. When S2 turns off at t10, 2) Input utility-line frequency: Fac= 60Hz Mode 8 ends. 3) Rated power of LED street-lighting module: Po = 144W 4) Rated voltage of LED street-lighting module: Vo = 36V. 5) Rated current of LED street-lighting module: Io = 4A. Fig.10. Mode 8 Mode 9 The capacitors CS1 and Cr provide energy to Lr, Lm, CS2, CB and LB2, and the capacitor Co still provides energy to the LED street-lighting module during Mode 9. When vds1 decreases to zero at t11, Mode 9 ends and Mode 1 begins again for the next switching period. Fig.11. Mode 9 V. SIMULATION ANG RESULTS Fig.12. Simulation circuit of single phase closed loop resonant converter All Rights Reserved © 2015 IJARTET 11 ISSN 2394-3777 (Print) ISSN 2394-3785 (Online) Available online at www.ijartet.com International Journal of Advanced Research Trends in Engineering and Technology (IJARTET) Vol. II, Special Issue XIII, March 2015 Fig.13. Measured switch voltage (ZVS) Fig.14. Measured voltage and resonant current Measured waveform of switching voltage vds2 along with the switching current ids2 and ZVS is obtained on the power switch S2. The measured voltage vds2 and resonant current iLr is shown in above Fig VI. CONCLUSION Although many solutions were offered for single-phase active PFC, three-phase active PFC was seldom considered. 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