9
Hindawi Publishing Corporation Mathematical Problems in Engineering Volume 2013, Article ID 912487, 8 pages http://dx.doi.org/10.1155/2013/912487 Research Article Designing a Single-Stage Inverter for Photovoltaic System Application M. T. Tsai, C. L. Chu, C. M. Mi, J. Y. Lin, and Y. C. Hsueh Southern Taiwan University of Science and Technology, No. 1, Nan-Tai Street, Yungkang District, Tainan City 710, Taiwan Correspondence should be addressed to M. T. Tsai; [email protected] Received 12 September 2013; Accepted 8 October 2013 Academic Editor: Teen-Hang Meen Copyright ยฉ 2013 M. T. Tsai et al. is is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. is paper focuses on a full-bridge high-frequency isolated inverter which is proposed for distributed photovoltaic power supply application. e researched system consists of a full-bridge high-frequency DC/DC converter with the proposed symmetric phase- shi๏ฌ… modulation algorithm to achieve the ZVS switching function and a line frequency unfolding bridge. It replaces the traditional two stages of independent control algorithms with a one-stage control to obtain high conversion e๏ฌƒciency. A TMS 320F2812 digital signal processor-based control technique is used to achieve the desired algorithm function for the grid-connected photovoltaic power system application. e researched system can have two operating methods depending on the applied situation. Finally, a prototype of 300 W with the maximum power point function is settled to verify the proposed idea. 1. Introduction Recently, renewable energy, such as wind power and photo- voltaic cell (PV), feeding the distributed power systems, has been increased and more visibile. For PV applications, since the conversion becomes more and more e๏ฌƒcient due to the di๏ฌ€erent existing conversion technologies and the decreasing price of the PV modules, it has become suitable for small- scale residential applications with a range below 1 kW [1โ€“ 6]. ere are many existing power inverter topologies for interfacing PV modules to the used terminal. Generally, a PV power system can be divided into stand-alone system and grid-connected system depending on whether it is parallel with the utility or not. For the stand-alone system, it usually needs batteries to give a supplement to the insu๏ฌƒcient photo- voltaic power. Stand-alone system is mainly used in the place without utility source or sparsely populated areas where the utility cannot supply energy with low cost. Grid-connected system is mainly used in the area where the utility can be served. Inverters connected to the grid involve two major functions, one is to ensure that the PV is operated with the maximum power point tracking (MPPT) and the other is to inject a sinusoidal current into the grid [7โ€“11]. Development of grid-connected photovoltaic power sup- ply system is divided into two categories, including cen- tralized converter type and microconverter type [1โ€“5]. e former uses multiple photovoltaic modules for string and/or parallel combination to concentrate the utility; such a frame- work is usually to adopt a stable DC bus design and it uses a large capacity of electrolyte capacitor to obtain a stable DC voltage; its advantages are more ๏ฌ‚exible than converter design, but with a worse operation performance for each module, while the latter, oppositely usually uses one or few photovoltaic modules to the utility, and the pulsating DC bus design and a small volume electrolyte capacitor are adopted. us, photovoltaic modules can have a better running perfor- mance. However, each team of photovoltaic modules requires a special convertor to transfer the energy to the electricity. A single-stage high-frequency converter topology for decentralized PV systems has been presented in this paper for small-scale residential applications. In contrast to the classic converter topologies the proposed scheme presents a high power density. e researched system consisted of a full- bridge high-frequency DC/DC converter with the proposed symmetric phase-shi๏ฌ… modulation algorithm to achieve the ZVS switching function and a DC/AC inverter which can

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Page 1: 912487

Hindawi Publishing CorporationMathematical Problems in EngineeringVolume 2013, Article ID 912487, 8 pageshttp://dx.doi.org/10.1155/2013/912487

Research ArticleDesigning a Single-Stage Inverter forPhotovoltaic System Application

M. T. Tsai, C. L. Chu, C. M. Mi, J. Y. Lin, and Y. C. Hsueh

Southern Taiwan University of Science and Technology, No. 1, Nan-Tai Street, Yungkang District, Tainan City 710, Taiwan

Correspondence should be addressed to M. T. Tsai; [email protected]

Received 12 September 2013; Accepted 8 October 2013

Academic Editor: Teen-Hang Meen

Copyright ยฉ 2013 M. T. Tsai et al.This is an open access article distributed under theCreativeCommonsAttribution License, whichpermits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

This paper focuses on a full-bridge high-frequency isolated inverter which is proposed for distributed photovoltaic power supplyapplication.The researched system consists of a full-bridge high-frequency DC/DC converter with the proposed symmetric phase-shift modulation algorithm to achieve the ZVS switching function and a line frequency unfolding bridge. It replaces the traditionaltwo stages of independent control algorithms with a one-stage control to obtain high conversion efficiency. A TMS 320F2812 digitalsignal processor-based control technique is used to achieve the desired algorithm function for the grid-connected photovoltaicpower system application. The researched system can have two operating methods depending on the applied situation. Finally, aprototype of 300W with the maximum power point function is settled to verify the proposed idea.

1. Introduction

Recently, renewable energy, such as wind power and photo-voltaic cell (PV), feeding the distributed power systems, hasbeen increased and more visibile. For PV applications, sincethe conversion becomes more and more efficient due to thedifferent existing conversion technologies and the decreasingprice of the PV modules, it has become suitable for small-scale residential applications with a range below 1 kW [1โ€“6]. There are many existing power inverter topologies forinterfacing PVmodules to the used terminal. Generally, a PVpower system can be divided into stand-alone system andgrid-connected system depending on whether it is parallelwith the utility or not. For the stand-alone system, it usuallyneeds batteries to give a supplement to the insufficient photo-voltaic power. Stand-alone system is mainly used in the placewithout utility source or sparsely populated areas where theutility cannot supply energy with low cost. Grid-connectedsystem is mainly used in the area where the utility can beserved. Inverters connected to the grid involve two majorfunctions, one is to ensure that the PV is operated with themaximum power point tracking (MPPT) and the other is toinject a sinusoidal current into the grid [7โ€“11].

Development of grid-connected photovoltaic power sup-ply system is divided into two categories, including cen-tralized converter type and microconverter type [1โ€“5]. Theformer uses multiple photovoltaic modules for string and/orparallel combination to concentrate the utility; such a frame-work is usually to adopt a stable DC bus design and it usesa large capacity of electrolyte capacitor to obtain a stableDC voltage; its advantages are more flexible than converterdesign, but with a worse operation performance for eachmodule, while the latter, oppositely usually uses one or fewphotovoltaic modules to the utility, and the pulsating DC busdesign and a small volume electrolyte capacitor are adopted.Thus, photovoltaicmodules can have a better running perfor-mance. However, each team of photovoltaicmodules requiresa special convertor to transfer the energy to the electricity.

A single-stage high-frequency converter topology fordecentralized PV systems has been presented in this paper forsmall-scale residential applications. In contrast to the classicconverter topologies the proposed scheme presents a highpower density. The researched system consisted of a full-bridge high-frequency DC/DC converter with the proposedsymmetric phase-shift modulation algorithm to achieve theZVS switching function and a DC/AC inverter which can

Page 2: 912487

2 Mathematical Problems in Engineering

200V

110โˆš2V

โˆ’110โˆš2V

Renewable

energy

DC/DCwith high

voltageoutput

DC/ACinverter Grid

(a)

110โˆš2V

110โˆš2V

โˆ’110โˆš2V

Renewable

energy

Grid

DC/DCwith

rectifiedsinusoidal

output

Unfolding

bridge

(b)

Figure 1: (a) Two-stage control-based PV system. (b) Single-stage control-based PV system.

Vin

S1 S3

S5 S6

S2 S4

Lr

Iin Vnยฑ

1:N:NLo1

Co VACCr

(a)

Vin

S1 S3 S5 S6

S2 S4

ยฑ VAC

In

Vn

1:N S6 S5

Lf

CfCinโˆ’

+

(b)

Figure 2: (a) The proposed single-stage control-based PV system architecture 1. (b) The proposed single-stage control-based PV system-architecture 2.

have two operating methods depending on the load charac-teristic. With the proposed control algorithm, it meets therequirement of a high efficiency conversion.

2. System Structure

PVpower system is roughly divided into twomajor categoriesisolated and nonisolated. This study was to investigate thedesign of high-frequency isolated structure. For such anarchitecture, it is basically divided into two control designsdepending on the availability large electrolyte capacitor, andcan be described as follows.

2.1. Comparison of Two-Stage and Single-Stage Control-BasedPV System. Two-Stage control based PV system basicallyconsists of a high-frequency DC/DC stage whose output isconnected to a stiff DC bus voltage which is with large elec-trolyte capacitors. Then the second DC/AC stage operatedin sinusoidal pulse-width modulation switching transfers theenergy to the utility. It can be shown in Figure 1(a). In contrastto this, the single-stage control based PV system basicallyconsists of a high-frequency DC/DC stage whose outputconnected to a pulsating DC bus voltage which is with noelectrolyte capacitors. Then an unfolding full-bridge inverter

switched in 60Hz transfers the energy to the utility. It can beshown in Figure 1(b).

2.2. Single-Stage Control Based PV System. The proposedsingle-stage control based PV system can be implementedin two ways as shown in Figures 2(a) and 2(b). These twoarchitectures have common characteristic of using pulse-link DC-AC convertor [6]; therefore, a pulsating waveformpresented in its DC output side.The difference between themis that the formerโ€™s output stage can do the PWM switchingin order to implement the nonunit power factor current,while the latter does not have this ability. When parallel tothe utility, the control responsibility of both architecturesin no change at the first stage, while the second stage isresponsible only for low frequency (e.g., 60Hz) switching tolower the switching losses. Under this situation, feeding anonunit power current into the main will cause a distortedcurrent waveform, and the distorted current can be solvedby a properly PWM switching algorithm for Figure 2(a) butcannot be fitted for Figure 2(b).

This study is focused on a single-stage control basedPV system shown in Figure 2, and a symmetric phase-shift control algorithm is adopted to replace the traditionalSPWM switching algorithm so as to achieve the zero-voltage

Page 3: 912487

Mathematical Problems in Engineering 3

S1

S4

S2

S6

S5

S3

Vtri

In

๐›ผ

2

Vds4

t = 0VT

๐›ผ

2

Vds2

Ids4

Ids2

t0 t1 t2 t3 t4 t5 t6

Vn

Vc

โˆ’Vc

Figure 3: The conducting status of Figure 2(a) in stand-alone oper-ation.

switching function. Also, two different switching modes willbe introduced to cope with the unity power factor currentdemand or non-unit power current demand.

3. Symmetric Phase-Shift Control Algorithm

Conventional full-bridge phase-shift converter uses the par-asitic capacitance on the switching elements and the leakageinductance existed in the high-frequency transformer to getthe zero voltage switching effect. The advantages includereduced switching loss and the switch stress. However, it issuitable for DC/DC converter and cannot satisfy the sinewave output requirement. In response to the requirementachieved by single-stage control, this paper proposes a sym-metric phase-shift control to fulfill the DC/AC function. Thecontrol algorithm is shown as follows.

In the case of Figure 1(a), the modulation functionachieved by ๐‘†

1โˆผ ๐‘†4before high frequency transformer, de-

noted as ๐ป๐น(๐‘ก), can be described in (1), where ๐›ผ is denoted

as the desired phase shift angle:

๐ป๐น(๐‘ก) =

{{{{{{{

{{{{{{{

{

+๐‘‰in,๐›ผ

2โ‰ค ๐‘ก โ‰ค๐‘‡๐‘ 

2โˆ’๐›ผ

2,

โˆ’๐‘‰in,๐‘‡๐‘ 

2+๐›ผ

2โ‰ค ๐‘ก โ‰ค ๐‘‡ โˆ’

๐›ผ

2,

0, elsewhere.

(1)

Then, the modulation function achieved by ๐‘†5โˆผ ๐‘†6after

high frequency transformer, denoted as ๐ป๐ต(๐‘ก), can be de-

scribed as

๐ป๐ต(๐‘ก) = (

1 0 โ‰ค ๐‘ก โ‰ค๐‘‡๐‘ 

2

โˆ’1๐‘‡๐‘ 

2โ‰ค ๐‘ก โ‰ค ๐‘‡

๐‘ 

). (2)

Thus, the primary voltage๐‘‰๐‘›and the control command๐‘‰

๐‘can

be shown as follows:

๐‘‰๐‘›= ๐‘‰in (1 โˆ’

2๐›ผ

๐‘‡๐‘ 

) ,

๐›ผ = 0, ๐‘‰๐‘›= ๐‘‰in,

๐›ผ =๐‘‡๐‘ 

2, ๐‘‰

๐‘›= 0,

๐›ผ = ๐‘‡๐‘ , ๐‘‰

๐‘›= โˆ’๐‘‰in,

๐‘‰๐‘= (1 โˆ’2๐›ผ

๐‘‡๐‘ 

) .

(3)

To obtain a sinusoidal output, the command๐‘‰๐‘(๐‘ก)

should be asin๐œ”๐‘ก waveform; that is:

๐‘‰๐‘(๐‘ก) = ๐‘‰

๐‘sin๐œ”๐‘ก. (4)

Therefore, the output after ๐‘†5โˆผ๐‘†6can be expressed as follows:

๐‘‰๐‘œ= ๐‘๐‘‰in๐‘‰๐‘

๐‘‰insin๐œ”๐‘ก. (5)

3.1. Stand-Alone Operation. In this situation, the PV invertershould be capable of supplying non-unit power factor cur-rent drawn by the load; thus only the structure shown inFigure 2(a) can fulfill the requirement, and Figure 3 shows theconducting status in this operation.

3.1.1. Interval (๐‘ก0โ‰ค ๐‘ก < ๐‘ก

1). In this status, ๐‘†

1and ๐‘†4are ON;

๐‘†2and ๐‘†3are OFF. The transformer primary voltage is equal

to the DC input voltage, and input current flows through thetransformer primary side and the switches to form a currentloop, making the power from the input source through thetransformer to the secondary side, and then through the ๐‘†

5

to the load. Figure 4(a) shows the energy transfer interval.

3.1.2. Interval (๐‘ก1โ‰ค ๐‘ก < ๐‘ก

3). As shown in Figure 4(b) in

this status, ๐‘†2and ๐‘†4are ON; ๐‘†

1and ๐‘†3are OFF. The energy

flows through ๐‘†2and the transformer primary side to form

a flywheel current loop, and the transformer primary voltage๐‘‰๐‘›is in short status. For the transformer secondary, ๐‘†

5is ON

at ๐‘ก1โ‰ค ๐‘ก < ๐‘ก

2and ๐‘†6is ON at ๐‘ก

2โ‰ค ๐‘ก < ๐‘ก

3.

3.1.3. Interval (๐‘ก3โ‰ค ๐‘ก < ๐‘ก

4). In this status, ๐‘†

2and ๐‘†

3are

ON; ๐‘†1and ๐‘†

4are OFF. The transformer primary voltage is

equal to the negative DC input voltage, and input currentflows through the transformer primary side and the switches

Page 4: 912487

4 Mathematical Problems in Engineering

Vin

S1 S3

S5 S6

S2 S4

Lr

Iinยฑ

1:N:NLo

CoRo

Cr

(a)

Vin

S1 S3

S5 S6

S2 S4

Lr

Iinยฑ

1:N:NLo

Co RoCr

(b)

Vin

S1 S3

S5 S6

S2 S4

Lr

Iinยฑ

1:N:N

Lo

Co Ro

Cr

(c)

S1 S3

S5 S6

S2 S4

Lr

ยฑ

1:N:N

Lo

CoRo

Vin IinCr

(d)

Figure 4: (a) Energy transfer interval I. (b) Energy flywheel interval I. (c) Energy transfer interval II. (d) Energy flywheel interval II.

S1

S4

S2

S3

Vc

โˆ’Vc

In

Vds4

VT

Vds2

Ids4

Ids2

t0 t1 t2 t3 t4

Vn

Figure 5: The conducting status due to Figure 2(b) structure.

to form a current loop, making the power from the inputsource through the transformer to the secondary side, andthen through the ๐‘†

6to the load. Figure 4(c) shows the energy

transfer interval.

3.1.4. Interval (๐‘ก4โ‰ค ๐‘ก < ๐‘ก

6). As shown in Figure 4(d) in

this status, ๐‘†1and ๐‘†3are ON; ๐‘†

2and ๐‘†4are OFF. The energy

flows through ๐‘†1and the transformer primary side to form

a flywheel current loop, and the transformer primary voltage

Page 5: 912487

Mathematical Problems in Engineering 5

Vin

S1 S3 S5 S6

S2 S4

VnยฑCin

S5S6

VAC

+

โˆ’

Lf

Cf

In

(a)

Vin

S1 S3 S5 S6

S2

S4

VnยฑCin

S5S6

+

โˆ’

VAC

Lf

Cf

In

(b)

Vin

S1 S3 S5 S6

S2

S4

VnยฑCin

S5S6

+

โˆ’

VAC

Lf

Cf

In

(c)

Vin

S1 S3S5 S6

S2 S4

VnยฑCin

S5S6

+VAC

Lf

Cf

In

(d)

Figure 6: (a) Energy transfer interval I. (b) Energy flywheel interval I. (c) Energy transfer interval II. (d) Energy flywheel interval II.

๐‘‰๐‘›is in short status. For the transformer secondary, ๐‘†

6is ON

at ๐‘ก4โ‰ค ๐‘ก < ๐‘ก

5and ๐‘†5is ON at ๐‘ก

5โ‰ค ๐‘ก < ๐‘ก

6.

3.2. Grid-Connected Operation. In this situation, the PVinverter should be capable of supplying unity power factorcurrent to the utility; thus both the structures shown inFigures 2(a) and 2(b) can fulfill the requirement, where thetransformer secondary power switches ๐‘†

5and ๐‘†6used as the

unfolding bridge and switching at 60HZ. An example basedon Figure 2(b) topology can be shown in Figures 5 and 6,where Figure 5 shows the conducting status in the proposedcontrol algorithm, and Figure 6 shows the four conductingstages.

3.2.1. Interval (๐‘ก0โ‰ค ๐‘ก < ๐‘ก

1). As shown in Figure 6(a), in this

status ๐‘†1and ๐‘†4are ON; ๐‘†

2and ๐‘†3are OFF. The transformer

primary voltage is equal to the DC input voltage, and inputcurrent flows through the transformer primary side and theswitches to form a current loop, making the power fromthe input source through the transformer to the secondaryside, then through the ๐‘†

5or ๐‘†6to the load dependent on the

positive or negative cycle.

3.2.2. Interval (๐‘ก1โ‰ค ๐‘ก < ๐‘ก

2). As shown in Figure 6(b), in

this status ๐‘†2and ๐‘†

4are ON; ๐‘†

1and ๐‘†

3are OFF. The energy

flows through ๐‘†2and the transformer primary side to form

a flywheel current loop, and the transformer primary voltage๐‘‰๐‘›is in short status.

3.2.3. Interval (๐‘ก2โ‰ค ๐‘ก < ๐‘ก

3). As shown in Figure 6(c), in this

status ๐‘†2and ๐‘†3are ON; ๐‘†

2and ๐‘†4are OFF. The transformer

primary voltage is equal to the negativeDC input voltage, andinput current flows through the transformer primary side andthe switches to form a current loop, making the power fromthe input source through the transformer to the secondaryside, and then through the ๐‘†

5or ๐‘†6to the load dependent on

the positive or negative cycle.

3.2.4. Interval (๐‘ก3โ‰ค ๐‘ก < ๐‘ก

4). As shown in Figure 6(d), in

this status ๐‘†1and ๐‘†

3are ON; ๐‘†

2and ๐‘†

4are OFF. The energy

flows through ๐‘†1and the transformer primary side to form

a flywheel current loop, and the transformer primary voltage๐‘‰๐‘›is in short status.

3.3. Implementation. A prototype of 300W due toFigure 2(b) structure has been settled to verify theproposed idea for stand-alone operation and grid-connectedoperation. The proposed DSP TMS320F2812 processor-based single-stage control block diagram dependent onthe operation condition can be shown in Figures 7(a) and7(b). Figure 7(a) shows the control block diagram for thestand-alone operation, and Figure 7(b) shows the controlblock diagram for the grid-connected operation. Figure 7(c)

Page 6: 912487

6 Mathematical Problems in Engineering

PWM1

PWM2

ADCIN01

ADCIN0218kHz

18kHz

9kHz

20 kHz

Vref

Kv

Voltageand

currentsence

amplifier

GPtimer1clock

XINT1

Zerocross

ABS BRF

PI

Sine table

Phase shifted controlS1 S2 S3 S4 S5 S6

io

Vo

Vs

โˆ’

+

โˆ’

+โˆ’

+

(a)

PVpowersource

+

โˆ’

In

MPPT

Cin

S1

S2

S3

S4

48:400

DSPTMS320

F2812

Irms

Current loop control

Zero crossing detector

VAC

Lf

Cf

Grid1

Vn

S5 S6

S6 S5

Vrms

โˆ’

+

Vin

Iin

(b)

Irms Current sensor

Iset +โˆ’

Currentcontroller

Vc Phaseshift

control

Sietable

Vrms Zerovoltagedetector

(c)

Vc

โˆ’Vc

DC k = โˆ’1

QS

R

SET

CLRQ

P1

P2

+โˆ’

S2

S1

S3

S4

QS

R Q

QS

R

SET

CLRQ

+โˆ’

+โˆ’

+โˆ’

+โˆ’

+โˆ’

+โˆ’

SET

CLR

(d)

Figure 7: (a) DSP-based control block diagram for the stand-alone operation. (b) DSP-based control block diagram for the grid-connectedoperation. (c) Current control loop. (d) Modulation strategy used for the grid-connected operation.

Page 7: 912487

Mathematical Problems in Engineering 7

Vs1

Vds4

Ids4

Vs4

Vs1,Vs4 : 10V/div Vds4 : 50V/div Ids4 : 10A/div t : 10๐œ‡s/div

Figure 8: The driving signals ๐‘‰๐‘ 1, ๐‘‰๐‘ 4, the corresponding voltage ๐‘‰ds4, and current ๐ผds4 of ๐‘†4.

(a)

Irms

Vrms

300W188W 200W 300W

(b)

Figure 9: The maximum power point tracking function in the proposed microinverter via a PV emulator manufactured by the Chromacompany, (a) the maximum power point operating at 200W, and (b) the tracking performance due to the PV power change of 300Wโ€“200Wโ€“300W.

Vn

In

Figure 10: The primary input voltage and current of the high-frequency transformer.

shows the current controller, and Figure 7(d) shows themodulation strategy for ๐‘†

1โˆผ ๐‘†4used for the grid-connected

operation.

4. Simulation and Experimental Results

The system parameters used in the prototype are shown inTable 1.

Figure 8 shows the experimental results, including thedriving signals of the switching devices, ๐‘†

1, ๐‘†4, and the

Table 1: The parameters used in the experimental system.

๐‘‰in 40โˆผ60V๐‘‰๐‘œ

110๐‘‰AC๐‘†1โˆผ ๐‘†6

IXTQ69N30๐ฟ๐‘“

220 uF๐ถ๐‘“

2.2 uFSwitching frequency 18 kHzOutput power 300W

corresponding voltage waveform and current waveformof ๐‘†4.

It shows that the switches can achieve ZVS function.Figure 9 shows the maximum power point tracking

function in the proposed microinverter via a PV emulatormanufactured by the Chroma company. The PV outputpower is set at 200W. It shows the proposed microinverteris operated at the maximum power related to the set point.

Figure 10 shows the primary input voltage and current ofthe high frequency transformer. It shows that no bias currentexisted there.

Figure 11 shows the inverter output voltage and currentin the case of stand-alone situation and the grid-connected

Page 8: 912487

8 Mathematical Problems in Engineering

Vo

Io

(a)

VoIo

(b)

Figure 11: The inverter output voltage and current, (a) the stand-alone operation, and (b) the grid-connected operation.๐‘‰

0: 100V/div.

๐ผ0: 5 A/div. ๐‘ก: 2.5ms/div.

situation. Figure 11(a) shows the stand-alone operation, andFigure 11(b) shows the grid-connected operation. It showsthe proposed micro inverter can achieve the inphase currentfunction due to the current control loop, and with low har-monics. The overall system efficiency is about 90%.

5. Conclusion

This paper discusses the steady-state behavior of the single-stage control-based inverter when controlled via a symmet-rical phase shift modulation. The single-stage control basedalgorithm to replace the traditional two-stage control in themicro inverter applications can reduce the system complexityand increase the reliability due to the lack of the electrolyticcapacitor. With the use of new symmetrical phase shiftcontrol, the ZVS switching performance can be achieved forthe proposed micro inverter so as to reduce the switchingstress and switching loss and thus improve the inverterโ€™soverall efficiency. The theoretical framework is validated bymeans of computer simulations and experimental results ona 300W prototype.

Acknowledgment

This work has been supported by National Science Council,Taiwan, under research project NSC101-2221-E-218-040.

References

[1] R.-J. Wai and W.-H. Wang, โ€œGrid-connected photovoltaic gen-eration system,โ€ IEEETransactions onCircuits and Systems I, vol.55, no. 3, pp. 953โ€“964, 2008.

[2] S. B. Kjaer, J. K. Pedersen, and F. Blaabjerg, โ€œA review of single-phase grid-connected inverters for photovoltaicmodules,โ€ IEEE

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