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A HIGH-EFFICIENCY MOSFET TRANSFORMERLESS INVERTER FOR NONISOLATED MICROINVERTER APPLICATIONS ABSTRACT: State-of-the-art low-power-level metal–oxide– semiconductor field-effect transistor (MOSFET)-based transformer less photovoltaic (PV) inverters can achieve high efficiency by using latest super junction MOSFETs. However, these MOSFET-based inverter topologies suffer from one or more of these drawbacks: MOSFET failure risk from body diode reverse recovery, increased conduction losses due to more devices, or low magnetic utilization. By splitting the conventional MOSFETbased phase leg with an optimized inductor, this paper proposes a novel MOSFET-based phase leg configuration to minimize these drawbacks. Based on the proposed phase leg configuration, a high efficiency singlephase MOSFET transformer less inverter is presented for the PV micro inverter applications. The pulse width modulation (PWM) modulation and circuit operation principle are then described. The common-mode and differential-mode voltage model is then presented and analyzed for circuit design. Experimental results of a 250Whardware prototype are shown to demonstrate the merits of the proposed transformerless inverter on nonisolated two-stage PV microinverter application. INTRODUCTION: With worldwide growing demand for electric energy, there has been a great interest in exploring photovoltaic (pv) sources. The pv microinverter has become a popular trend for its great flexibility in system installation and expansion, safety of low-input voltage, and high system-level energy harnessing under shading. Because it is not mandatory for pv micro inverters to have galvanic insulation, the nonisolated architecture, is an ideal choice for high efficiency design. Gu et al. Reported a nonisolated high boost ratio dc–dc converter, which boosts pv panel voltage to around 380 v dc-link voltages for 240 v grid voltage and achieves high efficiency over wide input voltage range. In order to achieve high system efficiency and minimize the system common-mode (cm) voltage, the secondary stage of the nonisolated pv microinverter requires a high efficiency transformerless inverter In recent years, there have been quite a few new transformerless PV inverters topologies, which eliminate traditional line frequency transformers to achieve lower cost and higher efficiency, and maintain lower leakage current as well. For high-power- level transformerless inverters, most of them adopt neutral point clamp (NPC) or T-type three-level inverter topologies, which require high dc-bus voltage and are not suitable for low power PV inverter application. For the lower power level transformerless inverters, most of the innovative topologies use super junction metal–oxide–semiconductor field-effect transistor (MOSFET) to boost efficiency. With super junction MOSFETs, the conduction and switching losses are lowered. However, with the poor reverse recovery from MOSFET’s slow body diode, MOSFETbased phase legs will have a risk of device failure, which is related to high dv/dt, di/dt and phase-leg shoot through from gating voltage false trigging on. In the following, state-of-the-art MOSFET-based transformerless inverter topologies will be reviewed and discussed according to their circuit topology, efficiency, MOSFET failure possibility from body diode reverse recovery, and magnetic utilization. The first and most influential one is the Highly Efficient and Reliable Concept (HERIC) inverter topology ., this circuit uses ac switches S5/D5 (or S6/D6) to decouple the PV panel from the grid during the current freewheeling period to reduce the CMvoltage. Topology uses one active switch and four diodes to replace the two active switches at the cost of higher conduction loss on freewheeling diodes. EXISTING SYSTEM: The topology called “highly efficient and reliable inverter concept” (heric), derives directly from the full-bridge converter, in which a bypass leg has been added in the ac side by means of two back-to-back igbts operating at grid frequency. The bypass branch has two important functions: decoupling the pv array from the grid (using a method called “ac decoupling”), avoiding the presence of high-frequency voltage components across it and preventing the reactive power exchange between the filter inductors and cin during the zero voltage state, thus increasing efficiency [2]. The converter operates as it follows during the positive half-cycle s+ remains connected, whereas s1 and s4 commutate at switching frequency in order to generate both active and zero vectors. When an active vector is present (s1 and s4 are on), current flows from the pv panels to the grid, while, when a zero vector occurs, s1 and s4 are switched off and the current flows through s+ and d-, this is the freewheeling situation. On the other hand, when the negative cycle is coming, s+ goes off and s- goes on, whereas s3 and s2 commutate at switching frequency. It means that an active vector is present when s3 and s2 are on, therefore the current flows from the pv panel towards the load, thus when s3 and s2 turn off, a zero voltage vector is present in the load, then current flows through s- and d+. PROPOSED SYSTEM: S1, s2, d1, d2, and lo1 make up one proposed phase leg and s3, s4, d3, d4, and lo4 make up another proposed phase leg; s5 and d5 provide a freewheeling loop for positive current; s6 and d6 provide a freewheeling loop for negative current. Phase leg splitting inductors lo1 and lo4 can be coupled together and filter inductors lo2 and lo3 can be coupled together. The phase-leg splitting inductors lo1 and lo4 have 50% utilization, but the filter inductors lo2 and lo3 have full utilization. The phase-leg splitting inductors lo1 and lo4 are only designed for di/dt suppression with a value much smaller than the filter inductance. In this paper, the total inductance of phase-leg splitting inductor is 86 μh, and the filter inductors lo2 and lo3 are 4.7 mh. So even though the phase-leg splitting inductors only have 50% utilization, the overall inductance utilization is over 98%. The proposed inverter almost achieves almost full utilization of magnetics. Thus, the cost and volume of magnetic can almost be reduced by half. In addition, the proposed inverter still does not need pwm dead-time, only has two devices in the conduction loss, and has no risk from reverse recovery of mosfet body diodes. ADVANTAGES: High efficiency Low cm voltage Improved magnetic utilization BLOCK DIAGRAM: TOOLS AND SOFTWARE USED: MPLAB – microcontroller programming. ORCAD – circuit layout. MATLAB/Simulink – Simulation APPLICATIONS: Photovoltaic (pv) sources. CONCLUSION: This paper proposes a MOSFET transformerless inverter with a novel MOSFET-based phase leg, which achieves: 1) high efficiency by using super junction MOSFETs and SiC diodes; 2) minimized risks from the MOSFET phase leg by splitting the MOSFET phase leg with optimized inductor and minimizing the di/dt from MOSFET body diode reverse recovery; 3) high magnetics utilization compared with previous high efficiency MOSFET transformerless inverters in [21], [22], [25], which only have 50% magnetics utilization. The proposed transformerless inverter has no dead-time requirement, simple PWM modulation for implementation, and minimized high-frequency CMissue. REFERENCES: [1] F. Blaabjerg, Z. Chen, and S. B. Kjaer, “Power electronics as efficient interface in dispersed power generation systems,” IEEE Trans. Power Electron., vol. 19, no. 5, pp. 1184–1194, Sep. 2004. [2] S. B. Kjaer, J. K. Pedersen, and F. Blaabjerg, “A review of singlephase grid-connected inverters for photovoltaic modules,” IEEE Trans. Ind. Appl., vol. 41, no. 5, p. 1292, Sep. 2005. [3] Q. Li and P. Wolfs, “A review of the single phase photovoltaic module integrated converter topologies with three different dc link configurations,” IEEE Trans. Power Electron., vol. 23, no. 3, pp. 1320–1333, May 2008. [4] Y. Xue, L. Chang, S. B. Kjaer, J. Bordonau, and T. Shimizu, “Topologies of singlephase inverters for small distributed power generators: An overview,” IEEE Trans. Power Electron., vol. 19, no. 5, pp. 1305–1314, 2004. [5] W. Yu, J. S. Lai, H. Qian, and C. Hutchens, “High-efficiency MOSFET inverter with H6-type configuration for photovoltaic non-isolated AC-module applications,” IEEE Trans. Power Electron., vol. 56, no. 4, pp. 1253–1260, Apr. 2011