Next Article in Journal
Thermodynamic, Exergetic and Thermoeconomic Analyses of Double-Effect LiBr–Water Absorption Refrigeration Systems with a 5 kW High Temperature PEMFC as Heat Source for Data Center Applications
Previous Article in Journal
Forecasting Daily Electricity Consumption in Thailand Using Regression, Artificial Neural Network, Support Vector Machine, and Hybrid Models
Previous Article in Special Issue
Transformer-Less Switched-Capacitor Quasi-Switched Boost DC-DC Converter
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Review

Topology Review of Three-Phase Two-Level Transformerless Photovoltaic Inverters for Common-Mode Voltage Reduction

1
Department of Electrical Engineering, Chonnam National University, Gwangju 61186, Korea
2
Faculty of Electrical and Electronics Engineering, Ho Chi Minh City University of Technology and Education, Ho Chi Minh City 700000, Vietnam
3
Faculty of Electrical Engineering Technology, Industrial University of Ho Chi Minh City, Ho Chi Minh City 700000, Vietnam
*
Authors to whom correspondence should be addressed.
Energies 2022, 15(9), 3106; https://doi.org/10.3390/en15093106
Submission received: 30 March 2022 / Revised: 17 April 2022 / Accepted: 21 April 2022 / Published: 24 April 2022
(This article belongs to the Special Issue Energy Conversion and Operation Technologies for Smart Grid)

Abstract

:
In grid-connected photovoltaic (PV) systems, a transformer is needed to achieve the galvanic isolation and voltage ratio transformations. Nevertheless, these traditional configurations of transformers increase the weight, size, and cost of the inverter while decreasing the efficiency and power density. The transformerless topologies have become a good solution. However, the problem is that commode-mode voltage and leakage current can occur via the stray capacitors between the PV array and the ground of the inverter. Various transformerless inverters have been introduced with different techniques, such as reducing the common-mode voltage or eliminating the leakage current. Furthermore, to introduce the development of transformerless PV inverters, especially in three-phase two-level inverter systems, this paper provides a comprehensive review of various common-mode voltage reduction three-phase two-level inverters.

1. Introduction

Nowadays, renewable energy sources play a key role in supporting the power system to adapt the ever-increasing load demand. Among the renewable energy sources, the PV source is considered as one of the most effective solutions due to its relatively small size, clean energy, noiseless operation, and simple installation [1,2,3,4]. To connect the PV array with a utility grid, grid-connected inverters are widely used for the PV systems and are divided into the transformer-based and transformerless topologies [4,5,6,7,8,9]. The use of a high-frequency transformer on the DC side or a low-frequency, bulky transformer in the AC side can be employed to ensure the safety issue with the galvanic isolation between the output and input sides [10,11,12]. Nevertheless, transformer-based topologies are heavy, high-cost, and high-loss. The efficiency of the transformerless inverter can improve by up to 2%. Therefore, transformerless topologies have been developed in both academic and industrial fields [13,14,15,16,17,18]. Voltage source inverters (VSIs), especially three-phase two-level transformerless topologies, are the most common solution to convert the DC voltage to AC voltage in any power system, with their merits of being low-cost, easy to implement, and mature technology. However, the disadvantage of transformerless topologies is the connection of the PV array to the grid without galvanic isolation. So, international agencies have regulated some broadly approved standards for PV inverters, which should be considered to avoid safety concerns. The main reason for these safety concerns is the presence of large stray capacitance (CPV) between the PV panel and the ground of the grid. As highlighted in Figure 1, a direct ground–current path may form between the grid and the PV panel. Due to the presence of large stray capacitance between the PV panel and grid grounds, the common-mode voltage (CMV) can appear, and the leakage current is originated from CMV fluctuations. Then, the leakage current flows through the ground and PV array, which leads to increased radiated electromagnetic emissions, higher current harmonics, and losses and low reliability of the transformerless, grid-connected PV transformerless inverter topologies [19,20,21]. Considering these issues, the leakage current should be carefully managed. The leakage current must be less than the VDE standard of 300 mA to prevent the unfavorable effects in VDE 0126-1-1. The leakage current can be suppressed by reducing the amplitude and frequency of the CMV or breaking the PV array from the grid on the DC side of the inverter system. In recent years, many approaches have been made to overcome the CMV and leakage current in transformerless PV inverters [21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38].
The SVM control method is generally implemented to control the traditional three-phase two-level H6 VSI. Figure 2 shows the circuit and SVM diagram of the traditional three-phase two-level H6 VSI. It can be seen that eight possible combinations are synthesized of six active and two zero voltage vectors, as depicted in Table 1. Moreover, the CMV can be defined as the average of the voltages between the three-phase voltages, A-N, B-N, and C-N, and (1) and the CMV in each state are calculated in Table 1.
V C M = V G N = V A N + V B N + V C N 3
There are several review papers reported in the literature which cover the topology modifications and PWM methods for CMV reduction in three-phase VSIs [27,37,38,39,40]. In the review study [27], the CMV in an electric drive fed by a conventional three-phase two-level inverter is described and a review of CMV reduction methods is presented. The PWM methods for CMV reduction in three-phase two-level transformerless inverters are discussed in [37,38,39,40] to demonstrate the effectiveness of the compared solutions. Generally, these review papers only focused on the traditional three-phase two-level transformerless inverters with a buck-type topology. Moreover, the prior-art solutions for traditional VSIs are not suitable for the impedance-source-based inverters system. Hence, the review solutions for CMV reduction in the impedance-source-based in VSIs are presented in [41]. However, not many different comparisons have been conducted in this review paper. Investigating the latest research in both traditional VSIs and impedance-source-based VSIs, the review and classification of three-phase two-level transformerless inverters have been studied in this paper to present a clear picture of the investigation of the three-phase two-level transformerless PV inverters for CMV reduction. For each category of three-phase two-level transformerless inverters, several general inverter topologies of them are illustrated, and each inverter has been examined from different perspectives, such as the number of components, modulation index operating range, CMV reduction, boosting voltage capability, etc. The rest of this paper is organized as follows. Section 2 presents the classification of three-phase two-level transformerless topologies. A broad classification and discussion of different traditional three-phase two-level transformerless inverter topologies are given in Section 3. Section 4 provides the structure of major impedance-source-networks-based topologies with the comparison between them based on the merits and demerits. Finally, Section 5 gives the concluding remarks.

2. Classification of Three-Phase Two-Level Transformerless Topologies for CMV Reduction

Compared with CSIs, the VSIs will be more dominant in the PV-grid-connected inverter systems because of their advantages of easy control, cost-effectiveness, and being a mature technology [42,43,44,45,46,47,48,49,50,51,52]. However, the traditional three-phase two-level voltage-source H6 inverter cannot provide the boost capability. Thus, an additional boost from a DC–DC converter or new topologies with added extra components can be used to boost the low input DC voltage to high DC-link voltage [53,54,55,56,57]. Moreover, a deadtime should be inserted in the H-bridge switches to avoid the short-circuiting of the DC-link bus. This leads to an increase in the THD value at the AC output voltage [58,59]. These days, single-stage, impedance-source inverter topologies [60,61,62,63,64,65,66,67,68,69,70] have been introduced and developed with buck-boost ability and improve reliability. In a transformerless PV inverter, the common mode voltage will be produced while the inverter is being worked and results in the high-leakage current on the capacitor CPV [71,72]. In order to suppress the leakage current, the common mode voltage should be reduced or kept constant. To reduce the CMV for the traditional three-phase two-level H6 VSIs, both the PWM control methods [30,31,32,33,34,35,36,37,38] and system topology reconfiguration [42,43,44,45,46,47,48,49,50,51,52,53,54,55,56,57] are introduced. In addition, the solutions for the CMV reduction of the impedance-source inverter topologies were also developed. Moreover, by considering the number of active switches in the impedance-source network, these inverters can be classified into passive types [71,72,73,74,75,76,77,78,79] and active types in [80,81,82,83]. As a result, the transformerless three-phase two-level VSIs with CMV reduction can be classified into the traditional VSI group and impedance-source-based group. The overview of the several existed topologies is summarized and presented in Figure 3. The comprehensive comparison and discussion will be presented in the following sections.

3. Traditional Voltage Source Topologies

3.1. Buck-Type Topologies

From the CMV values listed in Table 1, the CMV of the traditional three-phase two-level H6 VSI can be reduced to one high CMV level by only applying six active states. Various PWM technique modifications for CMV reduction have been presented. This section will briefly present some SVM methods, such as the traditional modulation-based CMV reduction methods. In the active zero-state SVM method introduced in [30,31], the zero states can be replaced by two opposite active states. The near-state SVM method is implemented with three adjoining states [32]. The traditional three-phase two-level H6 VSI with these SVM methods can effectively decreases the CMV amplitude to 33% of DC-link voltage. The active zero-state PWM and near-state PWM methods, and the remote-state SVM method in [33], can offer the constant CMV by using only the three active states in the odd active or even vectors. Moreover, the combination of other states can be applied to reduce the amplitude value of CMV, introduced in [34,35,36]. However, this solution limits modulation index range and output voltage quality, which reduces the output quality of the inverter. The overview of these control methods is also discussed in [37,38,39,40,41].
Moreover, the inverter structure can be changed and introduced by modifying some components for the CMV reduction, as shown in Figure 4. For example, the H7 topology was introduced in [42,43] to limit the CMV of VPN/3. An extra switch was added to positive DC input voltage to disconnect the inverter side and PV source during one zero vector when the inverter operated with the discontinuous SVM method. In addition, to eliminate two CMV levels in two zero vectors, a H8 topology with two additional switches was proposed in [44,45]. Two additional switches were controlled to float the inverter in zero states; the variation of CMV is VPN/3. In [46], H8 topology with a voltage-clamping network was proposed. The CMV did not change with the zero vectors by turning off two additional switches. Thus, the CMV can vary from VPN/3 to 2VPN/3. In addition, an improved H8 topology was also proposed in [47]. In the improved H8 topology, the CMV during zero states is kept constant at 2VPN/5, while it varies from VPN/3 to 2VPN/3 in the active states. In [48,49], the H10 topologies and corresponding modulation scheme with omitting zero vectors were introduced to keep the constant CMV. Moreover, a constant CMV can be given by adding a zero-voltage-state rectifier module to the H6 inverter [50]. In [51], the modulation strategy for a three-phase four-leg PV inverter was discussed to achieve the constant CMV. Therefore, the leakage current can be eliminated remarkably.

3.2. Boost-Type Topologies

Unlike the previous solutions, many three-phase two-level inverters are shown in Figure 5. They are based on a combination of different types of boost modules, and each has its unique characteristics. In [53], the H6 topology with a switched-capacitor voltage doubler and the novel SVM methods were proposed to limit the variation of CMV and offer the boosting ability, where the DC-link voltage of the inverter is always two times the input voltage. However, the topology in [53] produces bipolar output line-to-line voltage, and the linear modulation range is also limited. In addition, the proposed triple voltage boost inverter in [54] uses a voltage multiplier network to give the triple boosting voltage and keep the constant CMV. In [55,56], the three-phase H6 based-switched-capacitor inverters were presented to reduce the variation of CMV with one-third of DC-link voltage and also provided the boosting voltage. In the case of the introduced inverter in [55], the DC-link of the inverter can be one or two times of the input voltage depending on the state of the switched-capacitor circuit. On the contrary, the inverter in [56] is always given two times the input voltage. Like conventional four-leg topology, the four-leg inverter with adding boosting module in [57] can also achieve the constant CMV, and the DC-link of the proposed inverter is always two times the input voltage.
Table 2 presents the comparison of both buck-type and boost-type traditional three-phase two-level transformerless inverter topologies in terms of component count, modulation index range, boosting capability, and variation of CMV. Figure 6 highlights the comparison of the detailed component count with the number of switches, diodes, capacitors, and inductors. It can be seen that the boost-type topologies require more components when compared with other buck-type topologies. In terms of modulation index operating range, the majority of inverters can operate in the modulation index in full range. It is clear that some of the proposed new structures reviewed in this study are provided by the boosting voltage and very low or constant CMV. However, to overcome some of the limitations, other components should be added, which, in most cases, will increase the size and weight of the inverter package. It can be seen that all the mentioned inverters have their own advantages and disadvantages, as presented in Table 2. Thus, it is difficult to evaluate which inverter is more effective than the other. Nevertheless, there are several key points that should be kept in mind while choosing an inverter for grid-connected three-phase two-level transformerless PV applications.

4. Impedance-Source-Networks-Based Topologies

4.1. Passive-Type Topologies

Figure 7 presents the general structure of an impedance-source network three-phase, two-level VSI with possible switching devices depending on application requirements. The basic impedance-source network can be established as a combination of inductors, capacitors, diodes, and switches to improve the performance of the circuit. In the control method of the impedance-source-networks-based inverter topologies, the shoot-through states are used to create shoot-through immunity and reduce the deadtime in H-bridge legs. On the contrary with the traditional VSI topologies, the shoot-through states insertion causes very high peak-to-peak CMV in the impedance-source-networks-based inverter topologies [71,72,73,74,75,76,77,78,79,80,81,82,83]. To reduce the CMV of the impedance-source-networks-based inverter topologies, various topologies and modulation techniques will be reviewed in this section. In the shoot-through states, during which each switching cycle is added to the H-bridge, none of the CMV reduction SVM control methods are ideal for impedance-source inverter topologies. In [71], an NSSVM strategy was proposed for a three-phase Z-source inverter, as shown in Figure 8a. In this work, the diode in the positive terminal is reversed-bias while the shoot-through states are implemented. Then, the input voltage source and an inverter are isolated. Similar to the NSSVM in the traditional H6 VSI, the magnitude CMV of three-phase Z-source inverters can be decreased to VPN/3. Nevertheless, the modulation index operating range is narrow and followed the conventional NSSVM; in this case, it is operated within 0.66 and 1. In order to provide the constant CMV in the Z-source inverter topology, the Z-source inverter with four-leg was found and presented in [72,73], as shown in Figure 8b. By switching the fourth leg, the CMV variation is significantly limited. Nevertheless, this method will result in a high cost of the three-phase system. In the same way, the three-phase Z-source inverter was proposed in [74,75], with an additional diode in the negative terminal of the input voltage source, as shown in Figure 8c. An additional diode has a function to seperate the inverter and the PV array during shoot-through states. In this case, the CMV is kept constant by using odd vectors. The modulation index is operated up to 0.57.
Moreover, to improve the input current profile, the quasi-Z-source inverter and modified quasi-Z-source inverter based on SVM were proposed in [76,77,78,79]. In the case of references [76,77,78], by adding an inductor in the negative terminal of the PV panel, only three odd or even vectors were implemented to keep the constant CMV. However, similar to the RSSVM in the traditional H6 VSI, the linear modulation range is limited to a modulation index of 0.57 in these methods. In addition, a notch filter is considered in [79] to add to the inverter system as an output filter. The CMV waveform is reduced when compared with the conventional SVM method. However, the leakage current can be eliminated in this case.

4.2. Active-Type Topologies

There are close similarities in the topologies of the passive and active impedance-source inverters which show that with the high reliability with shoot-through immunity, the deadtime issues can be avoided. However, the size and weight of inverter systems in passive impedance-source inverters are still large because of using inductor and capacitor elements in the Z-source network [63,64,65,66,67,68,69,70]. In recent years, in order to decrease the size and weight of the impedance-source inverter system, research on active impedance-source inverter has been paying attention to fewer numbers of passive elements. However, the disadvantage of these inverters is required to use more numbers of switch and gate drivers. With the shoot-through states insertion, the CMV problem of these two types is quite similar. For instance, the modified quasi-switched boost inverter with an additional inductor was proposed in [80] and shown in Figure 9a. In this solution, an inductor is inserted between the negative input and Z-network. That provides to reduce one level of the CMV waveform. In addition, the novel AZSVM was modified with one more shoot-through vector to reduce the variation in CMV to VPN/3, and the modulation index can operate up to 1. In the same way, the modified active quasi-Z-source inverter in Figure 9b was proposed to achieve the CMV of VPN/3. In this solution, the zero vectors are not implemented with the NSSVM method. Nevertheless, the modulation index of this SVM method is limited, within [0.66, 1]. Moreover, the magnitude of CMV in these solutions is not very low and only equal to VPN/3. In order to reduce the high CMV levels of the shoot-through vectors and provide smaller magnitude CMV voltage, the new impedance-source inverter with two switched-boost networks has been introduced in [82] and depicted in Figure 9c. In this solution, two additional switches in the Z-network are controlled to reduce the magnitude of CMV to VPN/6 and improve the boost factor. However, a large number of components were used in the Z-network. Similar to the AZSVM in the method in [80], the modulation index operating of this inverter can be full range, from 0 to 1. Moreover, another method to suppress the leakage current is directly connecting the neutral of the grid to the negative input of the PV panel. The CMV will be zero and also immune to any high-frequency components. As a result, there is no leakage current in the inverter system. To provide the boosting voltage and achieve the common-ground between PV panel and the grid, the common-ground quasi-Z-source inverter is reported in [83], as shown in Figure 9d.
The comparison of both passive and active three-phase, two-level transformerless impedance-source-networks-based inverters, in terms of component count, input current profile, modulation index range, boost factor, and variation of CMV, has been given in Table 3.
Figure 10 depicts the comparison of the component count in detail. It can be observed that the active-type impedance-source topologies and four-leg ZSI require more components than other passive-type impedance-source topologies. The boost factor is also presented in Figure 11. The active-type impedance-source inverters in [81,82] can offer a higher boost voltage ability than the other inverters. From the CMV comparison in Table 3, which achieved the constant CMV, the majority of inverter topologies cannot utilize the full range of the modulation index, and the zero vectors have not been implemented in the SVM method. In addition, the number of components should be large. To solve the high CMV level caused by the shoot-through vectors, various solutions, such as reconfiguring by adding a component or modified SVM methods, are introduced. However, these topologies require a large number of components to provide the boosting voltage, and very low or constant CMV. The advantages and disadvantages of the different CMV reduction impedance-source-networks-based topologies are also highlighted in Table 3. It is also difficult to determine which solution is better than the other. Nevertheless, if compared with the traditional inverter, the impedance-source inverters can give a higher voltage gain and provide the shoot-through immunity. These inverters can be considered with competitive solutions in PV applications.

5. Conclusions

To present the investigation of the three-phase two-level transformerless PV inverters for CMV reduction, the major three-phase two-level transformerless topologies have been surveyed based on conversion functionality. In detail, these topologies were classified into two different categories: traditional VSIs and impedance-source-based VSIs. For a general comparison, the features of both traditional buck-type and boost-type three-phase two-level transformerless topologies for CMV reduction were summarized. In addition, to have a further overview of common-mode voltage reduction in three-phase two-level inverters single-stage impedance-source-based inverters are also discussed in this paper. Different topologies were examined, in terms of the number of devices, modulation index operating range, boost factor, and CMV reduction. This survey and classification will help researchers to comprehend all these three-phase two-level transformerless photovoltaic inverters for CMV reduction and to identify their pros and cons. From this point, it can be observed that the transformerless photovoltaic inverters have been a certain mature technology and successfully employed in the distributed photovoltaic grid-connected systems. A comprehensive review of control and modulation techniques for CMV reduction of three-phase two-level transformerless PV inverters will be presented in future research.

Author Contributions

Conceptualization, T.-D.D. and M.-K.N.; Methodology, T.-T.T.; Validation T.-D.D. and D.-V.V.; investigation, Y.-C.L.; writing—review and editing, T.-D.D. and M.-K.N.; resources and supervision, Y.-C.L. and J.-H.C. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Not applicable.

Conflicts of Interest

The authors declare no conflict of interest.

Abbreviations

PVPhotovoltaic
DCDirect current
ACAlternating current
VSIsVoltage source inverters
CSIsCurrent source inverters
CMVCommon-mode voltage
SVMSpace vector modulation
PWMPulse width modulation
THDTotal harmonic distortion
ZSIZ-source inverter
DSVMDiscontinuous space vector modulation
NSSVMNear-state space vector modulation
AZSVMActive zero-state space vector modulation
RSSVMRemote-state space vector modulation

References

  1. Almutairi, A.; Sayed, K.; Albagami, N.; Abo-Khalil, A.G.; Saleeb, H. Multi-Port PWM DC-DC Power Converter for Renewable Energy Applications. Energies 2021, 14, 3490. [Google Scholar] [CrossRef]
  2. Abramovitz, A.; Shmilovitz, D. Short Survey of Architectures of Photovoltaic Arrays for Solar Power Generation Systems. Energies 2021, 14, 4917. [Google Scholar] [CrossRef]
  3. Bughneda, A.; Salem, M.; Richelli, A.; Ishak, D.; Alatai, S. Review of Multilevel Inverters for PV Energy System Applications. Energies 2021, 14, 1585. [Google Scholar] [CrossRef]
  4. Subramaniam, U.; Bhaskar, S.M.; Almakhles, D.J.; Padmanaban, S.; Leonowicz, Z. Investigations on EMI Mitigation Techniques: Intent to Reduce Grid-Tied PV Inverter Common Mode Current and Voltage. Energies 2019, 12, 3395. [Google Scholar] [CrossRef] [Green Version]
  5. Nguyen, M.K.; Duong, T.D.; Lim, Y.C.; Kim, Y.J. Isolated boost DC-DC converter with three switches. IEEE Trans. Power Electron. 2018, 33, 1389–1398. [Google Scholar] [CrossRef]
  6. Duong, T.D.; Nguyen, M.K.; Tran, T.T.; Lim, Y.C.; Choi, J.H. Transformerless High Step-Up DC-DC Converters with Switched-Capacitor Network. Electronics 2019, 8, 1420. [Google Scholar] [CrossRef] [Green Version]
  7. Kouro, S.; Leon, J.I.; Vinnikov, D.; Franquelo, L.G. Grid-connected photovoltaic systems: An overview of recent research and emerging PV converter technology. IEEE Ind. Electron. Mag. 2015, 9, 47–61. [Google Scholar] [CrossRef]
  8. Nguyen, M.K.; Duong, T.D.; Lim, L.C. Switched-capacitor-based dual-switch high-boost DC-DC converter. IEEE Trans. Power Electron. 2018, 33, 4181–4189. [Google Scholar] [CrossRef]
  9. Duong, T.D.; Nguyen, M.K.; Tran, T.T.; Lim, Y.C.; Choi, J.H. Transformer-Less Switched-Capacitor Quasi-Switched Boost DC-DC Converter. Energies 2021, 14, 6591. [Google Scholar] [CrossRef]
  10. Mohamed Hariri, M.H.; Mat Desa, M.K.; Masri, S.; Mohd Zainuri, M.A.A. Grid-Connected PV Generation System-Components and Challenges: A Review. Energies 2020, 13, 4279. [Google Scholar] [CrossRef]
  11. Ali Khan, M.Y.; Liu, H.; Yang, Z.; Yuan, X. A Comprehensive Review on Grid Connected Photovoltaic Inverters, Their Modulation Techniques, and Control Strategies. Energies 2020, 13, 4185. [Google Scholar] [CrossRef]
  12. Jo, K.Y.; Duong, T.D.; Nguyen, Y.C.; Choi, J.H. Emerging Technologies in Power Systems. Electronics 2022, 11, 71. [Google Scholar] [CrossRef]
  13. Zhai, L.; Lin, L.; Zhang, X.; Song, C. The Effect of Distributed Parameters on Conducted EMI from DC-Fed Motor Drive Systems in Electric Vehicles. Energies 2017, 10, 1. [Google Scholar] [CrossRef] [Green Version]
  14. Monjo, L.; Sainz, L.; Mesas, J.J.; Pedra, J. Quasi-Z-Source Inverter-Based Photovoltaic Power System Modeling for Grid Stability Studies. Energies 2021, 14, 508. [Google Scholar] [CrossRef]
  15. Duong, T.D.; Nguyen, M.K.; Lim, Y.C.; Choi, J.H.; Wang, C.; Vilathgamuwa, M. Modeling and Control of a Discontinuous Quasi-Switched Boost Cascaded Multilevel Inverter for Grid-Tied Applications. In Proceedings of the 2020 IEEE Energy Conversion Congress and Exposition (ECCE), Detroit, MI, USA, 11–15 October 2020; pp. 3261–3265. [Google Scholar]
  16. Kerekes, T.; Teodorescu, R.; Liserre, M.; Klumpner, C.; Sumner, M. Evaluation of Three-Phase Transformerless Photovoltaic Inverter Topologies. IEEE Trans. Power Electron. 2009, 24, 2202–2211. [Google Scholar] [CrossRef]
  17. Tang, Y.; Yao, W.; Loh, P.C.; Blaabjerg, F. Highly Reliable Transformerless Photovoltaic Inverters with Leakage Current and Pulsating Power Elimination. IEEE Trans. Ind. Electron. 2016, 63, 1016–1026. [Google Scholar] [CrossRef]
  18. Yang, B.; Li, W.; Gu, Y.; Cui, W.; He, X. Improved Transformerless Inverter with Common-Mode Leakage Current Elimination for a Photovoltaic Grid-Connected Power System. IEEE Trans. Power Electron. 2012, 27, 752–762. [Google Scholar] [CrossRef]
  19. Julian, A.L.; Oriti, G.; Lipo, T.A. Elimination of common-mode voltage in three-phase sinusoidal power converters. IEEE Trans. Power Electron. 1999, 14, 982–989. [Google Scholar] [CrossRef]
  20. Son, Y.C.; Sul, S.K. Generalization of active filters for EMI reduction and harmonics compensation. IEEE Trans. Ind. Appl. 2006, 42, 545–551. [Google Scholar] [CrossRef]
  21. Ogasawara, S.; Ayano, H.; Akagi, H. Measurement and Reduction of EMI Radiated by a PWM Inverter-Fed AC Motor Drive Systems. IEEE Trans. Ind. Appl. 1997, 33, 1019–1026. [Google Scholar] [CrossRef] [Green Version]
  22. Wang, X.; Lin, H.; Yang, H. The Characteristics and Suppression of Common-Mode Current for Brushless Doubly Fed Generator System. IEEE Trans. Electromagn. Compat. 2020, 62, 2265–2276. [Google Scholar] [CrossRef]
  23. Akagi, H.; Hasegawa, H.; Doumoto, T. Design and performance of a passive EMI filter for use with a voltage-source PWM inverter having sinusoidal output voltage and zero common-mode voltage. IEEE Trans. Power Electron. 2004, 19, 1069–1076. [Google Scholar] [CrossRef]
  24. Heldwein, M.L.; Ertl, H.; Biela, J.; Kolar, J.W. Implementation of a Transformerless Common-Mode Active Filter for Offline Converter Systems. IEEE Trans. Ind. Electron. 2010, 57, 1772–1786. [Google Scholar] [CrossRef] [Green Version]
  25. Jeong, S.Y.; Shin, D.G.; Kim, J.G. A Transformer-Isolated Common-Mode Active EMI Filter without Additional Components on Power Lines. IEEE Trans. Power Electron. 2019, 34, 2244–2257. [Google Scholar] [CrossRef]
  26. Zheng, J.; Lyu, M.; Li, S.; Luo, Q.; Huang, K. Common-Mode Reduction SVPWM for Three-Phase Motor Fed by Two-Level Voltage Source Inverter. Energies 2020, 13, 3884. [Google Scholar] [CrossRef]
  27. Turzyński, M.; Musznicki, P. A Review of Reduction Methods of Impact of Common-Mode Voltage on Electric Drives. Energies 2021, 14, 4003. [Google Scholar] [CrossRef]
  28. Guo, X.; Wang, N.; Wang, B.; Lu, Z.; Blaabjerg, F. Evaluation of Three-Phase Transformerless DC-Bypass PV Inverters for Leakage Current Reduction. IEEE Trans. Power Electron. 2020, 35, 5918–5927. [Google Scholar] [CrossRef]
  29. Zalhaf, A.S.; Abdel-Salam, M.; Ahmed, M. An active common-mode voltage canceler for PWM converters in wind-turbine doubly-fed induction generators. Energies 2019, 12, 691. [Google Scholar] [CrossRef] [Green Version]
  30. Hava, A.M.; Un, E. Performance Analysis of Reduced Common-Mode Voltage PWM Methods and Comparison with Standard PWM Methods for Three-Phase Voltage-Source Inverters. IEEE Trans. Power Electron. 2009, 24, 241–252. [Google Scholar] [CrossRef]
  31. Un, E.; Hava, A.M. A Near-State PWM Method with Reduced Switching Losses and Reduced Common-Mode Voltage for Three-Phase Voltage Source Inverters. IEEE Trans. Ind. Appl. 2009, 45, 782–793. [Google Scholar] [CrossRef]
  32. Hava, A.M.; Um, E. A high-performance PWM algorithm for common-mode voltage reduction in three-phase voltage source inverters. IEEE Trans. Power Electron. 2011, 26, 1998–2008. [Google Scholar] [CrossRef]
  33. Cavalcanti, M.; Oliveria, K.C.D.; Farias, A.M.D.; Neves, F.A.S.; Azevedo, G.M.S.; Camboim, F.C. Modulation techniques to eliminate leakage currents in transformerless three-phase photovoltaic systems. IEEE Trans. Ind. Electron. 2010, 57, 1360–1368. [Google Scholar] [CrossRef]
  34. Hwang, S.I.; Kim, J.M. Opposite Triangle Carrier with SVPWM for Common-Mode Voltage Reduction in Dual Three Phase Motor Drives. Energies 2021, 14, 282. [Google Scholar] [CrossRef]
  35. Cacciato, M.; Caro, S.D.; Scarcella, G.; Scelba, G.; Testa, A. Improved space-vector modulation technique for common mode currents reduction. IET Power Electron. 2013, 6, 1248–1256. [Google Scholar] [CrossRef]
  36. Janabi, A.; Wang, B. Hybrid SVPWM scheme to minimize the common-mode voltage frequency and amplitude in voltage source inverter drives. IEEE Trans. Power Electron. 2019, 34, 1595–1610. [Google Scholar] [CrossRef]
  37. Hou, C.C.; Shih, C.C.; Cheng, P.T.; Hava, A.M. Common-Mode Voltage Reduction Pulsewidth Modulation Techniques for Three-Phase Grid-Connected Converters. IEEE Trans. Power Electron. 2013, 28, 1971–1979. [Google Scholar] [CrossRef]
  38. Chen, H.; Zhao, H. Review on pulse-width modulation strategies for common-mode voltage reduction in three-phase voltage-source inverters. IET Power Electron. 2016, 9, 2611–2620. [Google Scholar] [CrossRef]
  39. Xu, J.; Han, J.; He, R.; Wang, J.; Ali, M.; Tang, H. High-Frequency SiC Three-Phase VSIs With Common-Mode Voltage Reduction and Improved Performance Using Novel Tri-State PWM Method. IEEE Trans. Power Electron. 2019, 34, 1809–1822. [Google Scholar] [CrossRef]
  40. Xu, J.; Han, J.; He, R.; Wang, J.; Habib, S.; Tang, H. A Novel Scalar PWM Method to Reduce Leakage Current in Three-Phase Two-Level Transformerless Grid-Connected VSIs. IEEE Trans. Ind. Electron. 2020, 67, 3788–3797. [Google Scholar] [CrossRef]
  41. Yuan, J.; Yang, Y.H.; Blaabjerg, F. Leakage Current Mitigation in Transformerless Z-Source/Quasi-Z-Source PV Inverters: An Overview. In Proceedings of the 2019 IEEE Energy Conversion Congress and Exposition (ECCE), Baltimore, MD, USA, 29 September–3 October 2019; pp. 2603–2608. [Google Scholar]
  42. Freddy, T.K.S.; Rahim, N.A.; Hew, W.P.; Che, H.S. Modulation techniques to reduce leakage current in three phase tranformerless H7 photovoltaic inverter. IEEE Trans. Ind. Electron. 2015, 62, 322–331. [Google Scholar] [CrossRef]
  43. Negesse, B.B.; Park, C.H.; Lee, S.H.; Hwang, S.W.; Kim, J.M. Optimized modulation method for common mode voltage reduction in H7 inverter. Energies 2021, 14, 6409. [Google Scholar] [CrossRef]
  44. Jeong, W.S.; Lee, Y.S.; Lee, J.H.; Lee, C.H.; Won, C.Y. Space vector modulation (SVM) based common mode current (CMC) reduction method of H8 inverter for permanent magnet synchronous motor (PMSM) Drives. Energies 2022, 15, 266. [Google Scholar] [CrossRef]
  45. Rahimi, R.; Farhangi, S.; Farhangi, B.; Moradi, G.R.; Afshari, E.; Blaabjerg, F. H8 inverter to reduce leakage current in transformerless three phase grid connected photovoltaic systems. IEEE J. Emerg. Sel. Topics Power Electron. 2018, 6, 910–918. [Google Scholar] [CrossRef]
  46. Concari, L.; Barater, D.; Buticchi, G.; Concari, C.; Liserre, M. H8 inverter for common mode voltage reduction in electric drives. IEEE Trans. Ind. Appl. 2016, 52, 4010–4019. [Google Scholar] [CrossRef] [Green Version]
  47. Gupta, A.K.; Agrawal, H.; Agarwal, V. A novel three phase transformerless H8 topology with reduced leakage current for grid tied solar PV applications. IEEE Trans. Ind. Appl. 2019, 55, 1765–1774. [Google Scholar] [CrossRef]
  48. Arpan, H.; Vivek, A. Novel three phase H10 inverter topology with zero common mode voltage for three phase induction motor drive applications. IEEE Trans. Ind. Electron. 2022, 69, 7522–7525. [Google Scholar]
  49. Najafi, P.; Houshmand Viki, A.; Shahparasti, M.; Seyedalipour, S.S.; Pouresmaeil, E. A novel space vector modulation scheme for a 10 switch converter. Energies 2020, 13, 1855. [Google Scholar] [CrossRef] [Green Version]
  50. Guo, X.; Zhang, X.; Guan, H.; Kerekes, T.; Blaabjerg, F. Three phase ZVR topology and modulation strategy for transformerless PV system. IEEE Trans. Power Electron. 2019, 34, 1017–1021. [Google Scholar] [CrossRef] [Green Version]
  51. Guo, X.; He, R.; Jian, J.; Lu, Z.; Sun, X.; Guerrero, J.M. Leakage current elimination of four leg inverter for transformerless three phase PV systems. IEEE Trans. Power Electron. 2016, 31, 1841–1846. [Google Scholar] [CrossRef] [Green Version]
  52. Guo, X.; Zhou, J.; He, R.; Jia, X.; Rojas, C.A. Leakage current attenuation of a three phase cascaded inverter for transformerless grid connected PV systems. IEEE Trans. Ind. Electron. 2018, 65, 676–686. [Google Scholar] [CrossRef]
  53. Tran, T.T.; Nguyen, M.K.; Duong, T.D.; Choi, J.H.; Lim, Y.C.; Zare, F. A switched capacitor voltage doubler based boost inverter for common mode voltage reduction. IEEE Access 2019, 7, 98618–98629. [Google Scholar] [CrossRef]
  54. Tran, T.T.; Nguyen, M.K.; Ngo, V.Q.B.; Nguyen, H.N.; Duong, T.D.; Lim, Y.C.; Choi, J.H. A three phase constant common mode voltage inverter with triple voltage boost for transformerless photovoltaic system. IEEE Access 2020, 8, 166692–166702. [Google Scholar] [CrossRef]
  55. Hota, A.; Mohammad, M.Q.; Kirtley, J.L.; Vivek, A. Novel switched capacitor boost inverter configuration for three phase induction motor driven home appliances. IEEE Trans. Ind. Appl. 2021, 57, 1450–1458. [Google Scholar] [CrossRef]
  56. Hota, A.; Vivek, A. A Novel three phase induction motor drive with voltage boosting capability low current THD and low common-mode voltage. In Proceedings of the 2020 IEEE International Conference on the Power Electronics Drives and Energy Systems (PEDES), Jaipur, India, 16–19 December 2020; pp. 1–4. [Google Scholar]
  57. Kharan, S.; Somasekhar, V.T. An Integrated Four-leg Three-phase Transformerless PV Inverter with Voltage Boosting Capability. In Proceedings of the 2020 IEEE International Conference on Power Electronics, Drives and Energy Systems (PEDES), Jaipur, India, 16–19 December 2020; pp. 1–5. [Google Scholar]
  58. Peng, F.Z. Z-source inverter. IEEE Trans. Ind. Appl. 2003, 39, 504–510. [Google Scholar] [CrossRef]
  59. Liu, Y.; Ge, B.; Abu, R.H.; Sun, D. Comprehensive modeling of single-phase quasi-Z-source photovoltaic inverter to investigate low frequency voltage and current ripple. IEEE Trans. Ind. Electron. 2015, 62, 4194–4202. [Google Scholar] [CrossRef]
  60. Siwakoti, Y.P.; Peng, F.Z.; Blaabjerg, F.; Loh, P.C.; Town, G.E. Impedance-Source Networks for Electric Power Conversion Part I: A Topological Review. IEEE Trans. Power Electron. 2015, 30, 699–716. [Google Scholar] [CrossRef]
  61. Nguyen, M.K.; Lim, Y.C.; Park, S.J. A Comparison Between Single Phase Quasi Z Source and Quasi Switched Boost Inverters. IEEE Trans. Ind. Electron. 2015, 62, 6336–6344. [Google Scholar] [CrossRef]
  62. Duong, T.D.; Nguyen, M.K.; Lim, Y.C.; Choi, J.H.; Mahinda, D.V. A comparison between quasi Z source inverter and active quasi Z source inverter. In Proceedings of the 2019 10th International Conference on Power Electronics and ECCE Asia (ICPE 2019-ECCE Asia), Busan, Korea, 27–30 May 2019; pp. 1–6. [Google Scholar]
  63. Nguyen, M.K.; Le, T.V.; Park, S.J.; Lim, Y.C. A Class of Quasi-Switched Boost Inverters. IEEE Trans. Ind. Electron. 2015, 62, 1526–1536. [Google Scholar] [CrossRef]
  64. Barath, J.N.; Soundarrajan, A.; Stepenko, S.; Husev, O.; Vinnikov, D.; Nguyen, M.K. Topological Review of Quasi-Switched Boost Inverters. Electronics 2021, 10, 1485. [Google Scholar] [CrossRef]
  65. Nguyen, M.K.; Duong, T.D.; Lim, Y.C.; Choi, J.H.; Vilathgamuwa, D.M.; Walker, G.R. DC-Link quasi-switched boost inverter with improved PWM strategy and its comparative evaluation. IEEE Access 2020, 8, 53857–53867. [Google Scholar] [CrossRef]
  66. Nguyen, M.K.; Choi, Y.O. Maximum boost control method for single-phase quasi-switched-boost and quasi-Z-source inverters. Energies 2017, 10, 553. [Google Scholar] [CrossRef]
  67. Nguyen, M.K.; Duong, T.D.; Lim, Y.C.; Kim, Y.G. Switched-Capacitor Quasi-Switched Boost Inverters. IEEE Trans. Ind. Electron. 2017, 65, 5105–5113. [Google Scholar] [CrossRef]
  68. Hossameldin, A.A.; Abdelsalam, A.K.; Ibrahim, A.A.; Williams, B.W. Enhanced Performance Modified Discontinuous PWM Technique for Three-Phase Z-Source Inverter. Energies 2020, 13, 578. [Google Scholar] [CrossRef] [Green Version]
  69. Duong, T.D.; Nguyen, M.K.; Lim, Y.C.; Choi, J.H.; Vilathgamuwa, D.M. SiC-Based Active Quasi-Z-Source Inverter with Improved PWM Control Strategy. IET Power Electron. 2019, 12, 3810–3821. [Google Scholar] [CrossRef]
  70. Nguyen, M.K.; Duong, T.D.; Lim, Y.C.; Choi, J.H. High Voltage Gain Quasi-Switched Boost Inverters with Low Input Current Ripple. IEEE Trans. Ind. Inform. 2018, 15, 4857–4866. [Google Scholar] [CrossRef]
  71. Erginer, V.; Sarul, M.H. A novel reduced leakage-current modulation technique for Z source inverter used in photovoltaic systems. IET Power Electron. 2014, 7, 496–502. [Google Scholar] [CrossRef]
  72. Guo, X.; Yang, Y.; He, R.; Wang, B.; Blaabjerg, F. Leakage current reduction of three phase Z source three level four leg inverter for transformerless PV system. IEEE Trans. Power Electron. 2019, 34, 6299–6308. [Google Scholar] [CrossRef]
  73. Guo, X.; Yang, Y.; He, R.; Wang, B.; Blaabjerg, F. Transformerless Z source four leg PV inverter with leakage current reduction. IEEE Trans. Power Electron. 2019, 34, 4343–4352. [Google Scholar] [CrossRef]
  74. Bradaschia, F.; Cavalcanti, M.C.; Ferraz, P.E.P.; Neves, F.A.S. Modulation for three phase transformerless Z source inverter to reduce leakage currents in photovoltaic systems. IEEE Trans. Ind. Electron. 2011, 58, 5385–5395. [Google Scholar] [CrossRef]
  75. Ferraz, P.E.P.; Bradaschia, F.; Cavalcanti, M.C.; Neves, F.A.S.; Azevedo, G.M.S. A modified Z-source inverter topology for stable operation of transformerless photovoltaic systems with reduced leakage currents. In Proceedings of the XI Brazilian Power Electronics Conference, Natal, Brazil, 11–15 September 2011; pp. 615–622. [Google Scholar]
  76. Liu, W.; Yang, Y.; Kerekes, T. Modified Quasi-Z-Source Inverter with Model Predictive Control for Constant Common-Mode Voltage. In Proceedings of the ICPE-ECCE Asia, Busan, Korea, 27–30 May 2019; pp. 1–6. [Google Scholar]
  77. Liu, W.; Yang, Y.; Kerekes, T.; Liivik, E.; Vinnikov, D.; Blaabjerg, F. Common-Mode Voltage Analysis and Reduction for the Quasi-Z-Source Inverter with a Split Inductor. Appl. Sci. 2020, 10, 8713. [Google Scholar] [CrossRef]
  78. Noroozi, N.; Zolghadri, M.R. Three phase quasi Z source inverter with constant common mode voltage for photovoltaic application. IEEE Trans. Ind. Electron. 2018, 65, 4790–4798. [Google Scholar] [CrossRef]
  79. Noroozi, N.; Yaghoubi, M.; Zolghadri, M.R. A modulation method for leakage current reduction in a three phase grid tie quasi Z source inverter. IEEE Trans. Power Electron. 2019, 34, 5439–5450. [Google Scholar] [CrossRef]
  80. Duong, T.D.; Nguyen, M.K.; Tran, T.T.; Lim, Y.C.; Choi, J.H.; Wang, C. Modulation Techniques for a Modified Three-Phase Quasi-Switched Boost Inverter with Common-Mode Voltage Reduction. IEEE Access 2020, 8, 160670–160683. [Google Scholar] [CrossRef]
  81. Nguyen, M.K.; Choi, Y.O. Modulation Technique for Modified Active Quasi-Z-Source Inverter with Common-Mode Voltage Reduction. Electronics 2021, 10, 2968. [Google Scholar] [CrossRef]
  82. Duong, T.D.; Nguyen, M.K.; Tran, T.T.; Vo, D.V.; Lim, Y.C.; Choi, J.H. Three-Phase Impedance-Source Inverter with Common-Mode Voltage Reduction. IEEE Access 2021, 9, 164510–164519. [Google Scholar] [CrossRef]
  83. Kharan, S.; Akash, S.; Rajeev, K.S. Transformerless Common Ground Quasi-Z-Source Three Phase Inverter for PV Applications. In Proceedings of the IECON 2020 The 46th Annual Conference of the IEEE Industrial Electronics Society, Singapore, 18–21 October 2020; pp. 1935–1940. [Google Scholar]
Figure 1. Typical three-phase transformerless VSI configuration using an L-filter.
Figure 1. Typical three-phase transformerless VSI configuration using an L-filter.
Energies 15 03106 g001
Figure 2. Traditional three-phase two-level voltage-source H6 inverter: (a) H6 inverter topology; (b) space vector modulation (SVM) diagram.
Figure 2. Traditional three-phase two-level voltage-source H6 inverter: (a) H6 inverter topology; (b) space vector modulation (SVM) diagram.
Energies 15 03106 g002
Figure 3. Classification of three-phase, two-level inverter topologies.
Figure 3. Classification of three-phase, two-level inverter topologies.
Energies 15 03106 g003
Figure 4. CMV reduction topologies. (a) H7 topology [42,43], (bd) H8 topologies [44,45,46,47], (e,f) H10 topology [48,49], (g) ZVR topology [50], and (h) four-leg topology [51].
Figure 4. CMV reduction topologies. (a) H7 topology [42,43], (bd) H8 topologies [44,45,46,47], (e,f) H10 topology [48,49], (g) ZVR topology [50], and (h) four-leg topology [51].
Energies 15 03106 g004aEnergies 15 03106 g004b
Figure 5. CMV reduction topologies with boosting capability. (a) Switched-capacitor voltage-doubler inverter [53], (b) triple-voltage boost inverter [54], (c,d) switched-capacitor-based inverters [55,56], (e) boost inverter with four-leg [57].
Figure 5. CMV reduction topologies with boosting capability. (a) Switched-capacitor voltage-doubler inverter [53], (b) triple-voltage boost inverter [54], (c,d) switched-capacitor-based inverters [55,56], (e) boost inverter with four-leg [57].
Energies 15 03106 g005
Figure 6. The components for topologies enlisted in Table 2.
Figure 6. The components for topologies enlisted in Table 2.
Energies 15 03106 g006
Figure 7. General structure of impedance-source-networks-based three-phase transformerless VSI.
Figure 7. General structure of impedance-source-networks-based three-phase transformerless VSI.
Energies 15 03106 g007
Figure 8. Passive impedance-source topologies for CMV reduction. (a) ZSI [71], (b) four-leg ZSI [72,73], (c) modified-ZSI [74,75], (d) qZSI [76,77].
Figure 8. Passive impedance-source topologies for CMV reduction. (a) ZSI [71], (b) four-leg ZSI [72,73], (c) modified-ZSI [74,75], (d) qZSI [76,77].
Energies 15 03106 g008
Figure 9. Active impedance-source topologies for CMV reduction. (a) MqSBI [80], (b) modified-AqZSI [81], (c) ISI [82], (d) and common-ground AqZSI [83].
Figure 9. Active impedance-source topologies for CMV reduction. (a) MqSBI [80], (b) modified-AqZSI [81], (c) ISI [82], (d) and common-ground AqZSI [83].
Energies 15 03106 g009
Figure 10. The components for topologies enlisted in Table 3.
Figure 10. The components for topologies enlisted in Table 3.
Energies 15 03106 g010
Figure 11. Comparison of boost factor.
Figure 11. Comparison of boost factor.
Energies 15 03106 g011
Table 1. Common-mode voltage of traditional H6 topology.
Table 1. Common-mode voltage of traditional H6 topology.
Switching StateBridge StatesCMV Value
M00000
M1100VPN/3
M21102VPN/3
M3010VPN/3
M40112VPN/3
M5001VPN/3
M61012VPN/3
M7111VPN
Table 2. Comparison of different CMV reduction traditional VSIs topologies.
Table 2. Comparison of different CMV reduction traditional VSIs topologies.
TopologyComponent CountModulation IndexBoost FactorCMVCharacteristic
SDCLAdvantageDisadvantage
Figure 4a [42]70070 to 11VPN/3
Minimum components
Full range of modulation index
Low CMV
No boosting capability
Figure 4b [45]80000 to 11VPN/3
Simple structure
Full range of modulation index
Low CMV
No boosting capability
Figure 4c [46]82300 to 11VPN/3
Full range of modulation index
Low CMV
No boosting capability
Requires more components
Figure 4d [47]80000 to 11VPN/3
Simple structure
Full range of modulation index
Low CMV
No boosting capability
Figure 4e [48]100200 to 110
Constant CMV
Full range of modulation index
Requires ten switches
No boosting capability
Figure 4f [49]100000 to 110
Constant CMV
Full range of modulation index
Requires ten switches
No boosting capability
Figure 4g [50]912200 to 110
Constant CMV
No boosting capability
High number of components
Limits modulation index
Figure 4h [51]80110.66 to 110
Simple structure
Constant CMV
No boosting capability
Limits modulation index
Figure 5a with DSVM [53]82200 to 12VPN/3
Double of input voltage
Full range of modulation index
Requires more components
Low CMV
Figure 5a with NSSVM [53]82200.66 to 12VPN/6
Double of input voltage
Very low CMV
Requires more components
Limits modulation index
Figure 5a with RSSVM [53]82200 to 0.5720
Double of input voltage
Constant CMV
Requires more components
Limits modulation index
Figure 5b [54]104300 to 130
Triple of input voltage
Constant CMV
Full range of modulation index
High number of components
Figure 5c [55]81100 to 11 or 2VPN/3
Double of input voltage
Full range of modulation index
Requires more components
Low CMV
Figure 5d [56]91110 to 12VPN/3
Double of input voltage
Full range of modulation index
Requires more components
Low CMV
Figure 5e [57]81220 to 120
Double of input voltage
Constant CMV
Full range of modulation index
Requires more components
S, D, L, and C are the number of switches, diodes, inductors, and capacitors, respectively.
Table 3. Comparison of different CMV reduction impedance-source-networks-based topologies.
Table 3. Comparison of different CMV reduction impedance-source-networks-based topologies.
TopologyComponent CountModulation IndexBoost FactorCMVCharacteristic
SDCLAdvantageDisadvantage
Figure 8a [71]61220.66 to 11/(1 − 2D)VPN/3
Low number of components and not require additional switch
Discontinuous input current
Limits modulation index
Not high voltage gain
Low CMV
Figure 8b [73]82330 to 11/(1 − 2D)0
Full range of modulation index
Constant CMV
High number of components
Discontinuous input current
Not high voltage gain
Figure 8c [74]62220 to 0.571/(1 − 2D)0
Low number of components and not require additional switch
Constant CMV
Discontinuous input current
Limits modulation index
Not high gain
Figure 8d [76]61230 to 0.571/(1 − 2D)0
Low number of components and not require additional switch
Continuous input current
Constant CMV
Limits modulation index
Not high voltage gain
Figure 9a [80]81120 to 11/(1 − 2D)VPN/3
Low number of components
Continuous input current
Full range of modulation index
Require additional switch
Not high voltage gain
Low CMV
Figure 9b [81]82220 to 12/(1 − 3D)VPN/6
Continuous input current
Full range of modulation index
High voltage gain
High number of components and require additional switch
Low CMV
Figure 9c [82]72230.66 to 11/(1 − 3D + D2)VPN/3
Continuous input current
Full range of modulation index
High voltage gain
Very low CMV
High number of components and require additional switch
Figure 9d [83]92320 to 11/(1 − 2D)0
Continuous input current
Full range of modulation index
Constant CMV
High number of components and require additional switch
Not high voltage gain
S, D, L, and C are the number of switches, diodes, inductors, and capacitors, respectively.
Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Share and Cite

MDPI and ACS Style

Duong, T.-D.; Nguyen, M.-K.; Tran, T.-T.; Vo, D.-V.; Lim, Y.-C.; Choi, J.-H. Topology Review of Three-Phase Two-Level Transformerless Photovoltaic Inverters for Common-Mode Voltage Reduction. Energies 2022, 15, 3106. https://doi.org/10.3390/en15093106

AMA Style

Duong T-D, Nguyen M-K, Tran T-T, Vo D-V, Lim Y-C, Choi J-H. Topology Review of Three-Phase Two-Level Transformerless Photovoltaic Inverters for Common-Mode Voltage Reduction. Energies. 2022; 15(9):3106. https://doi.org/10.3390/en15093106

Chicago/Turabian Style

Duong, Truong-Duy, Minh-Khai Nguyen, Tan-Tai Tran, Dai-Van Vo, Young-Cheol Lim, and Joon-Ho Choi. 2022. "Topology Review of Three-Phase Two-Level Transformerless Photovoltaic Inverters for Common-Mode Voltage Reduction" Energies 15, no. 9: 3106. https://doi.org/10.3390/en15093106

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop