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1.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395 -0056 Volume: 04 Issue: 03 | Mar -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2726 Soft-Switching Two-Switch Resonant Ac-Dc Converter Aqulin Ouseph1, Prof. Kiran Boby2, , Prof. Dinto Mathew3 1PG Scholar,Department of Electrical and Electronics Engineering, Mar Athanasius College of Engineering, Kothamangalam, Kerala, India 2,3Assistant Professor, Department of Electrical and Electronics Engineering, Mar Athanasius College of Engineering, Kothamangalam, Kerala, India ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract - In AC to DC converters, power factor has significant importance. Most power converters and equipments are developed to have power factor correction technology to improve their performance. A soft-switching two-switch resonant AC- DC converter with high power factor is presented. In this converter, a boost PFC circuit is integrated with a soft-switching resonant converter in order to achieve high power factor. This topology provide low component stress, high frequency operation, zero voltage switching, and applicability under a wide range of input and output conditions. The voltage across the main switches is confined to the dc-link voltage and the energy of the transformer leakage inductance is also recycled. Soft- switching operation of main switches and output diodes is achieved in a resonant manner and the switching losses are significantly reduced. Thus, the overall efficiency is improved. Key Words: Power factor correction(PFC), Soft switching, Resonant converter, Boost converter 1. INTRODUCTION The power supply unit is an essential circuit block in all electronic equipment. It is the interface between the AC mains and the rest of the functional circuits of the equipment. These functional circuits usually need power at one or more fixed dc voltage levels. Switched mode power supplies (SMPS) are most commonly used for powering electronic equipment since they provide an economical, efficient and high power density solution compared to linear regulators. In order to conserve energy, high overall power conversion efficiency is required. However, conventional AC/DC switched mode power supplies introduce some adverse effects on the AC side [1]. Examples of such effects are, distortion of input current/voltage, input voltage dip due to the presence of bulk capacitors and electromagnetic interference (EMI) due to high frequency switching. 2. SOFT-SWITCHING TWO-SWITCH RESONANT AC-DC CONVERTER Soft-switching two-switch resonant AC-DC converter with high power factor merges a boost converter and a two switch resonant converter. The circuit diagram of the converter is shown in figure 1. The boost PFC circuit is designed to operate in discontinuous conduction mode (DCM) to achieve a high power factor. The maximum voltages across main switches and clamping diodes are confined to the dc-link voltage Vdc. The secondary side consists of an output capacitor and a voltage doubler with a resonant tank. The voltage of output diodes are clamped to Vo and so it has no high spike voltage due to voltage doubler topology. Soft-switching operation of main switches and output diodes is achieved due to resonance between transformer leakage inductance and a resonant capacitor and critical conduction mode (CRM) operation of a two switch resonant converter. CRM operation reduces switching losses of main switches at their turn-on and zero-current switching (ZCS) of the output diodes reduces the switching losses and alleviates reverse recovery problem of output diodes. In addition, the energy stored in leakage inductance and magnetizing inductance of the transformer is recycled. The boost PFC cell is composed of a boost inductor Lb, reverse-blocking diode Db, and a main switch S1. In the two-switch resonant DC-DC module, the transformer T1 is modeled as the magnetizing inductance Lm, the leakage inductance Lk, and an ideal transformer with a turns ratio of n:1. To simplify the total transformer leakage inductance, Lk is referred to the secondary side. The capacitor Cdc is a DC bus capacitor. The snubber diodes D1 and D2 are cross-connected across the main switches S1, S2, and the primary winding. The operation of the converter in one switching period TS can be divided into six modes.
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International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395 -0056 Volume: 04 Issue: 03 | Mar -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2727 3. OPERATION OF CONVERTER Prior to Mode 1, main switches S1, S2 and diodes D1, D2, and D02 are off. Diode D01 is conducting. Inductor currents iLm and is approach zero at t0. Fig-1: Soft-switching two-switch resonant AC-DC converter Mode: 1 At t0, when voltage VS1 is a minimum value, both switches S1 and S2 are turned on at the same time. This is called near zero-voltage switching (ZVS), and it minimizes the power dissipation at turn-on. Since the boost inductor voltage VLb is Vin, the boost inductor current iLb increases linearly. Snubber diodes D1 and D2 are reverse-biased as VD1 = VD2 = Vdc. Since the voltage VLm across the inductor Lm is Vdc, the inductor current iLm increases linearly. In the secondary of T1, with the turn-on of S1 and S2, output diode D02 starts to conduct, and resonance occurs between the leakage inductance Lk and the capacitor C1. Output diode D01 is reverse-biased as V0. Fig- 2(a) Mode 1 Mode: 2 At t1, when the leakage inductance current iLk reaches zero by resonance between Lk and C1, this mode begins. Zero-current turn-off of diode D02 is achieved. The inductance current iLm increases linearly from i1. At the end of this mode, the inductor currents iLm arrive at their maximum value. In the Secondary of the transformer T1, the leakage inductance current iLk is zero. Hence, output diodes D01 and D02 are turned off. Output diode D01 is reverse-biased and output diode D02 is reverse biased.
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International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395 -0056 Volume: 04 Issue: 03 | Mar -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2728 Fig-2(b) Mode 2 .Mode: 3 At t2, both switches S1 and S2 are turned o_ at the same time. Since there is leakage inductance at the primary of the transformer T1, snubber diodes D1 and D2 are turned on by the current in the leakage inductance. Hence, the voltage VLm across the inductor Lm is Vdc. The inductor current iLm decreases linearly from i1 .Output diode D01 is turned on by the voltage of the secondary of the transformer T1. The inductor current iLk decreases linearly. At the end of this mode, snubber diode D1 arrives at zero, and inductor current iLm arrives at the value i2. Since snubber diodes D1 and D2 are turned on, main switch voltages VS1 and VS2 are clamped to Vdc. Fig-2(c) Mode 3 Mode: 4 At t3, when the snubber diode current iD1 reaches zero, this mode begins. However, snubber diode D2 is not turned off by the reverse-blocking diode Db. Therefore, main switch voltages VS1 is Vdc. At the end of this mode, boost inductor current iLb arrives at zero. The voltage VLm across inductor Lm is reflected the voltage of the secondary of the transformer T1. Fig-2(d) Mode 4 Mode: 5 At t4, when the boost inductor currents reach zero, this mode begins. Snubber diodes D1 and D2 are turned off. Fig-2(e) Mode 5
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International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395 -0056 Volume: 04 Issue: 03 | Mar -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2729 Mode: 6 At t5, the magnetizing inductance current iLm falls to zero, and output diode D01 is turned off under the ZCS condition. Then the voltages of main switches VS1 and VS2 decrease non linearly. Fig-2(f) Mode 6 4. SIMULATION MODELS AND RESULTS In this simulation work, Soft-Switching Two-Switch Resonant AC-DC Converter with PFC circuit is done by using Psim. In the two-switch resonant DC-DC module, the transformer T1 is modeled as the magnetizing inductance Lm, the leakage inductance Lk, and an ideal transformer with a turn ratio of n:1. Simulation parameters of Four phase interleaved buck converter are shown in table.3.1. Figure 3 shows the Psim model of the Soft-Switching Two-Switch Resonant AC-DC Converter with High Power Factor. 130V AC input is provided to the circuit and two MOSFETS are used. The gate signals to the MOSFETS are generated using PWM technique. Gate pulse for the switch can be generated by comparing a sawtooth and a constant. In Psim sawtooth of required frequency, 90 kHz is compared with a constant using a relational operator. Whenever repeating sequence is less than the constant, it will output a high value and if constant is smaller, it will output a low value. By varying the value of constant, duty ratio of MOSFET can be controlled. Switching pulses generated is applied to the switches of the converter. Figure 4 shows the simulated waveforms of the input voltage and input current, power factor respectively. The measured input voltage is 130 V and the output voltage is about 44.5 V. The measured power factor is about 0.9. Figure 5 shows input voltage, rectified voltage and voltage across capacitor. Table 1 Simulation Parameters PARAMETERS VALUES Supply Voltage 130 v Output Power 60W Switching Frequency 90KHz Inductor Lf 1.29mH Capacitor Cin 0.57 µF Inductor Lb 355 µH Capacitor Cdc 100µF Capacitor Cf 0.1 µF Transformer Lm = 1.48mH Lk = 0.25 µH 9:1 Capacitor C1 3.3 µF
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International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395 -0056 Volume: 04 Issue: 03 | Mar -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2730 Fig-3 Psim Model of two switch Resonant converter Fig-4 (a) Input Voltage, (b) Input Current and (c) Power Factor Fig-5 (a) Vac, (b) Vin and (c) Vdc Soft-switching operation of main switches and output diodes is achieved due to resonance between transformer leakage inductance and a resonant capacitor and critical conduction mode (CRM) operation of a two switch resonant converter. CRM operation reduces switching losses of main switches at turn-on of them and zero-current switching (ZCS) of the output diodes reduces also switching losses and alleviates reverse recovery problem of output diodes. It is shown in figure 6. Figure 7 indicate corresponding voltage stress of main MOSFETs. Figure 10 shows the simulated waveforms of iLb and VLb under 60W load conditions at 130 V ac. Since the phase of the input current is similar to that of the input line voltage, a high power factor is achieved.
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International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395 -0056 Volume: 04 Issue: 03 | Mar -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2731 Fig-6 Critical conduction mode operation Fig-7 Voltage across switches and diodes Fig-8 Power Factor Figure 9 shows the soft-switching waveforms of D01 and D02. Current circulating through secondary output diode Do1, naturally decreases to zero; the secondary output diode Do1 turns off under condition of zero current, and reverse recovery does not occur. The proposed converter obtains full range ZCS operations at heavy load condition. In figure 9, it can be seen that output diodes D01 and D02 operate in ZCS. The resonance between Lk and C1 ends before the turn-on of D01. Since voltage VD01 is maintained at zero after current iD02 arrives at zero, the turn-off loss of output diode D02 is almost zero, and the ZCS operation of D02 is achieved. After the current of output diode D01 reaches zero, the output diode D01 is turned off. Hence, the turn-off loss of output diode D01 is seen to be almost zero, and ZCS operation of D01 is achieved. In addition, the reverse recovery of output diodes D01 and D02 is significantly alleviated.
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International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395 -0056 Volume: 04 Issue: 03 | Mar -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2732 Fig-9 ZCS operation of diodes Fig-10 Current through Lb and Voltage across Lb It can be seen that resonance between Lk and C1 occurs, and the resonant current flows through output diode D02 during turn-on of the main switches S1 and S2. Main switch voltage VS1 is well clamped around Vdc. 5. CONCLUSIONS In the switching two-switch resonant AC-DC converter with PFC circuit, the boost PFC circuit operates in DCM. So a high power factor is achieved. Also the control circuit for the converter is simple. Voltage stress of main switches and diodes is reduced by utilizing two-switch structure and the voltage doubler of output stage. Moreover, the absorbed energy from the leakage inductor is reprocessed by the DC-DC module. Due to CRM operations of DC-DC module, switching losses of main switches are significantly reduced. Also, ZCS operation of output diodes is achieved by resonance manner. Therefore, the proposed converter alleviates the reverse-recovery losses of the output diodes. Hence, the converter provides high efficiency. Two-switch resonant AC-DC converter with PFC circuit achieves high power factor about 0.91. REFERENCES [1] Dunisha Wijeratne, Gerry Moschopoulos , A Two-Switch AC-DC Buck-Boost Quasi Resonant Front-End Converter", Applied Power Electronics Conference and Exposition , 2013 [2] H. S. Athab, D.C. Lu, and K. Ramar, A Single-Switch AC/DC Flyback Converter Using a CCM/DCM Quasi-Active Power Factor Correction Front-End, IEEETrans. Ind. Electron, Nov.2012. [3] Y. Wang, Y. Guan, X. Liang, W. Wang, and D. Xu, Two-stage LED street lighting system based on a novel single-stage AC/DC converter, IET Power Electronics, Jun. 2014. [4] H. S. Ribeiro and B. V. Borges, High-Performance Voltage-Fed ACDC Full-Bridge Single-Stage Power Factor Correctors with a Reduced DC Bus Capacitor, IEEE Trans. Power Electron. , June 2014.
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International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395 -0056 Volume: 04 Issue: 03 | Mar -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 2733 [5] C.A. Cheng, H.-L. Cheng, and T.Y. Chung, A Novel Single-Stage High-Power- Factor LED Street-Lighting Driver With Coupled Inductor, IEEE Trans. Ind. Appl., vol. 50 no. 5, pp. 3037 - 3045, Sep./Oct. 2014. [6] N. Golbon, and G. Moschopoulos, A Low-Power ACDC Single-Stage Converter With Reduced DC Bus Voltage Variation, IEEE Trans. Power Electron., Vol. 27, no. 8, pp.3714-3724, Aug. 2012. [7] Sin-Woo Lee, Hyun-Lark Do Soft-Switching Two-Switch Resonant AC-DC Converter with High Power Factor IEEE transactions on industrial electronics, Volume: 63, Issue: 4, 2016 [8] H. S. Athab and D.C. Lu, A High-Efficiency AC/DC Converter With Quasi-Active Power Factor Correction, IEEE Trans. Power Electronics, vol. 25 no. 5, pp.1103 1109, May 2010. [9] S.Y. Cho, I.O. Lee, J.-E. Park, and G. W. Moon, Two-stage Configuration for 60W Universal-line AC-DC Adapter, in Proc. IEEE IECON, 2012, pp. 1445-1450. 17 Soft-Switching Two-Switch Resonant AC-DC Converter with High Power Factor [10] J.E. Park, J.W. Kim, B. H. Lee, and G. W. Moon, Design on Topologies for High Efficiency Two-stage AC-DC Converter, in Proc. IEEE EECE Asia, 2012, pp.257-262. [11] A. Abasian, H. Farzaneh-fard, and S. Madani, Single stage soft-switching ac/dc converter without any extra switch, IET Power Electron., Vol. 7, no. 3, pp.745- 752, Mar. 2014.
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