Next Article in Journal
Speed Range Extension of Dual-Stator PM Machine Using Multi-Mode Winding Switching Strategy
Next Article in Special Issue
A General Equivalent Modeling Method for DFIG Wind Farms Based on Data-Driven Modeling
Previous Article in Journal
Methods of Large-Scale Capture and Removal of Atmospheric Greenhouse Gases
Previous Article in Special Issue
Comprehensive Comparison of a High-Speed Permanent Magnet Synchronous Motor Considering Rotor Length–Diameter Ratio
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

A Novel Model-Free Predictive Control for T-Type Three-Level Grid-Tied Inverters

1
School of Electrical Engineering and Automation, Anhui University, Hefei 230601, China
2
State Key Laboratory of Operation and Control of Renewable Energy & Storage Systems, China Electric Power Research Institute, Beijing 100192, China
3
School of Internet, Anhui University, Hefei 230601, China
4
Department of Electrical Engineering, Tsinghua University, Beijing 100190, China
*
Authors to whom correspondence should be addressed.
Energies 2022, 15(18), 6557; https://doi.org/10.3390/en15186557
Submission received: 28 July 2022 / Revised: 28 August 2022 / Accepted: 6 September 2022 / Published: 8 September 2022
(This article belongs to the Special Issue Energy, Electrical and Power Engineering 2021-2022)

Abstract

:
The model-free predictive control (MFPC) scheme is an effective scheme to enhance the parameter robustness of model predictive control. However, the MFPC scheme can be affected by the current gradient updating frequency. This paper proposes an improved MFPC scheme for a T-type three-level inverter. First, a novel current gradient updating method is designed to estimate all current gradients per control period, which uses the current gradient relationship between different voltage vectors and eliminates the effect of current gradients updating stagnation. Moreover, a sector judgment method based on the current gradient is proposed. Redundant small vectors are accurately judged and the computational burden is greatly reduced. Finally, simulation and experimental comparisons on a T-type three-level inverter verify the effectiveness of the proposed MFPC scheme.

1. Introduction

In recent years, grid-tied inverters, including two-level grid-tied inverters and multi-level grid-tied inverters, have been widely applied in various new energy generation systems, such as wind power generation systems [1] and photovoltaic power generation systems [2]. As the crucial interface between renewable energy generation systems and the grid, the grid-tied inverters are needed to meet the various requirements with better steady-state performance, faster dynamic performance, higher reliability, and so on [3,4]. Although two-level inverters are commonly used because of their flexible control and reliable operation, they also have some problems such as high harmonics. Compared to two-level inverters, multi-level inverters have many advantages. Among them, the T-type three-level inverter has been studied by many scholars because of its advantages of low output harmonic, low switching loss, and high efficiency [5,6].
With the increasing application of T-type three-level inverters, various control schemes have also been developed. In particular, model predictive control (MPC) schemes have been studied in T-type three-level inverters, with the advantages of high-speed response, comprehensive control schemes, and multi-objective control ability [7,8,9]. However, the control performance of MPC schemes mainly depends upon the accuracy of model parameters [10]. Many methods have been designed to improve the parameter robustness of MPC. System parameters are identified online to reduce parameter errors [11,12,13]. The disturbances generated by inaccurate parameters are calculated and compensated in the prediction [14,15]. In these studies, it is essential to tune parameters in different observers, which increases the calculation burden in traditional processors. Moreover, an MPC based on sum of squares optimization has been developed in [16], which improves output performance by formulating the largest possible region of attraction for the considered equilibrium point and guaranteeing the stability of the Lyapunov function. Recently, model-free predictive control (MFPC) has been reported to overcome this challenge by providing robust and accurate state predictions without a complete model of the system.
Various MFPC schemes have been reported based on the ultra-local model [17,18], the auto-regressive with exogenous input (ARX) model [19], and the look-up table (LUT) [20,21,22,23,24,25,26,27,28,29,30,31]. The model-free predictive control (MFPC) scheme based on LUT was firstly introduced in [20] for permanent magnet synchronous motor (PMSM) drives, which is a computationally light yet very effective scheme. This scheme uses the current gradient of each voltage vector to predict currents. However, the current gradients of remaining voltage vectors keep the old values, which is considered as the current gradient updating stagnation effect. In the most serious case, the long-term stagnation effect can affect the stability of the control system.
To improve the updating frequency of current gradients, an MFPC scheme based on minimum updating frequency is proposed to update each gradient within the specified time [21]. The implementation process is that, if a voltage vector is not used in the past predefined frequency, it will be forcibly used in the next period and its current gradient will be updated. However, this updating method [21] affects the control performance since the non-optimal voltage vector is used frequently. In [22,23], the remaining current gradients are estimated according to the updated current gradients of the used voltage vector in the past three times. This method is effective only when the voltage vectors of the past three consecutive periods are different from each other; otherwise, the update can stagnate. In [24], the current gradients of all unused voltage vectors are estimated by using the current gradient relationship between different voltage vectors. Nevertheless, the updating can be affected when the applied vectors are the same for two consecutive periods. In [25,26,27,28,29], multi-vector MFPC is studied, in which two or three current gradients of the two or three applied voltage vectors are updated by using multiple adaptive sampling points. Although the updated number of current gradients increases with the increase in the number of applied voltage vectors, the stagnation effect still exists. The MFPC scheme is used in the three-level inverter-fed interior PMSM system [30], and all the current gradients are divided into seven categories. Each type of current gradient is updated according to the amplitude relationship of the corresponding voltage vector. However, among the 27 current gradients corresponding to the 27 voltage vectors of the three-level inverter system, up to six current gradients can be updated. In [31], the extended adjacent state scheme is used to reduce the possible number of remaining gradients, then the measured current gradient is used to update the remaining current gradients.
The stagnation effect becomes more obvious as the number of voltage vectors increases when the MFPC scheme is used in a T-type three-level grid-tied inverter system. To enhance the parameter robustness of predictive control, eliminate the current gradient updating stagnation effect, and improve the efficiency of voltage vector optimization, this paper proposes an improved MFPC scheme. The main contributions are shown below.
(1)
A simplified look-up table (LUT) is designed. The redundant vector formed by two or three voltage vectors is considered as one corresponding current gradient. Hence, the number of LUTs decreased from 27 to 19.
(2)
A novel current gradient updating method is proposed to eliminate the stagnation effect caused by the conventional updating method. The current gradient relationship between different voltage vectors is derived, so all the current gradients can be estimated in each period.
(3)
A sector judgment method based on the current gradient is proposed. The proposed judgment method avoids using mathematical models to calculate the reference voltage. Hence, the number of candidate voltage vectors is reduced from 27 to 3, and the calculation speed is greatly improved.
The contents of this paper are organized as follows. In Section 2, the topology, vectors, and conventional MPC scheme are reviewed. In Section 3, the proposed scheme is introduced in detail. In Section 4, the proposed MFPC scheme is validated. In Section 5, the conclusion is given.

2. Conventional MPC Scheme

2.1. Topology and Voltage Vectors

The topology of the T-type three-level grid-tied inverter studied in this paper is shown in Figure 1, where udc is the dc-link voltage, and C1 and C2 are the upper and lower dc-link capacitors, respectively. O is the neutral point of dc-link capacitors and the zero-potential reference point. iC1 and iC2 are the current of C1 and C2, respectively. ig is the output current. It can be seen from Figure 1 that each T-type three-level inverter bridge arm contains four switching tubes, which are S1~S4. There are three switching modes, including P, O, and N modes, based on the different switching combinations. All bridge arms share the neutral point of dc-link capacitors.
There are 27 voltage vectors that can be generated by a three-phase three-level inverter, as shown in Figure 2. The specific positions in Figure 2 corresponding to multiple space vectors are called redundant vectors, whose output characteristics are equivalent. According to the amplitude of the voltage vector, the 27 switching states can be divided into a zero vector (PPP, OOO, NNN), small vector (POO, PPO, OPO, OPP, OOP, ONN, OON, NON, NOO, NNO, ONO), medium vector (PON, OPN, NPO, NOP, ONP, PNO), and large vector (PNN, PPN, NPN, NPP, NNP, PNP).

2.2. Conventional Predictive Model

The principle of the conventional MPC scheme has been studied in many papers. Firstly, the mathematical model based on the LR-filtered three-level inverter connecting to grids in the α-β coordinate system can be expressed as
L d i g d t = u x R i g e g
where ux = [u, u]T, ig = [i, i]T, and eg = [e, e]T represent the output voltage vectors of the inverter, output current vectors, and grid voltage vectors, respectively. L represents the filter inductance and R represents the stray resistance.
The discrete model of the inverter can be expressed as
i g ( k + 1 ) = i g ( k ) + T s L [ u x ( k ) R i g ( k ) e g ( k ) ]
where Ts is the control period.
The voltage vector selected in the last control period can be used to calculate the prediction current ig(k + 1) by (2). Then, all the voltage vectors shown in Figure 2 can be further used to calculate prediction currents igx(k + 2) by (3).
i g x ( k + 2 ) = ( 1 R T s L ) i g ( k + 1 ) + T s L [ u x ( k + 1 ) e g ( k + 1 ) ]
Finally, to evaluate the control performance of each voltage vector, a cost function shown in (4) is defined. The voltage vector that minimizes the cost function is used as the optimal vector and applied to the next control period.
G x = ( i r e f ( k + 2 ) i g x ( k + 2 ) ) 2
where iref(k + 2) are the reference currents.
In a three-level inverter control system, in addition to the output current, the neutral point voltage needs to be controlled. To avoid the design of weighting factor values when multiple control targets exist, MPC schemes without weighting factors have been proposed. In the MPC scheme without weighting factors, the P-type small vectors (POO, PPO, OPO, OPP, OOP) are considered as candidate vectors when the capacitor voltage uc1uc2, and the N-type small vectors (ONN, OON, NON, NOO, NNO, ONO) are considered as candidate vectors when the capacitor voltage uc1 < uc2. The control block diagram of MPC is shown in Figure 3.
However, the prediction currents are affected when model parameters are mismatched with the controller parameters. The prediction currents with parameter errors can be expressed as
i g e r r ( k + 1 ) = i g ( k ) + T s L + Δ L u x ( k ) ( R + Δ R ) i g ( k ) e g ( k )
where ∆L represents the inductance error between its actual value and its controller value, and ∆R represents the resistance error between its actual value and its controller value. Hence, it is important to enhance the parameter robustness of predictive control.

3. The Proposed MFPC Scheme

To eliminate the dependence on model parameters, an improved MFPC scheme based on a novel current gradient updating method is proposed in this section, including the basic principle of MFPC, the current gradient updating stagnation effect analysis, the proposed current gradient updating method, the sector judgment method, and the implementation steps.

3.1. Basic Principle of MFPC

In the MFPC scheme, the mathematical model (1) can be rewritten as [17]
Δ i x ( k 1 ) = T s L ( u x ( k 1 ) e g ( k 1 ) R i g ( k 1 ) )     = i g ( k ) i g ( k 1 )  
where ∆ix(k − 1) = [∆i(k − 1), ∆i(k − 1)]T are the current gradients of the applied voltage vector ux(k − 1). Although the switching states of redundant vectors are different, their coordinate components are the same. The multiple current gradients corresponding to redundant vectors are considered to be consistent. For example, voltage vector u1 corresponds to two switching states of ONN and POO, so the current gradient corresponding to the two states is uniformly defined as ∆i1. Hence, nineteen current gradients ∆ix are stored in the look-up table (LUT) for current predictions, as shown in Table 1.
Then, the prediction currents at the (k + 1)th instant and the (k + 2)th instant can be calculated based on (7) and (8), respectively.
i g x ( k + 1 ) = i g ( k ) + Δ i x ( k )
i g x ( k + 2 ) = i g x ( k + 1 ) + Δ i x ( k + 1 )
Finally, the optimal voltage vector uop selected by cost function (4) is applied in the next control period.

3.2. Current Gradient Updating Stagnation Effect Analysis

It is obvious that the current prediction of MFPC is based on the current gradients which directly affect the accuracy of current prediction and the result of optimal voltage vector selection. The current gradients of applied voltage vectors are calculated based on (6) in the conventional MFPC scheme [20], however, the updating of the remaining current gradients stagnates. When the MFPC scheme is used in a three-level inverter system, the stagnation effect can be more obvious with the increasing number of voltage vectors, which not only affects the current performance but also affects the control of the neutral point voltage.
To reduce the updating stagnation effect, various current gradient updating methods have been reported in [21,22,23,24,30]; however, the updating stagnation is still existing. Hence, it is necessary to design an updating method to totally eliminate the stagnation effect.

3.3. The Proposed Current Gradient Updating Method

In the proposed updating method, sampling points are set before switching states in each control period to avoid the current spikes. Based on (6), the relationship between the current gradient of remaining voltage vector ∆iy and the current gradient of applied voltage vector ∆ix at (k − 1)th instant and (k − 2)th instant can be expressed as (9) and (10), respectively.
Δ i y ( k 1 ) Δ i x ( k 1 ) = T s L ( u y ( k 1 ) u x ( k 1 ) )
Δ i y ( k 2 ) Δ i x ( k 2 ) = T s L ( u y ( k 2 ) u x ( k 2 ) )
The filter inductance L can be considered as a constant when Ts is short enough. Then, Ts/L of (9) and (10) can be eliminated by the division between (9) and (10), and the relationship between the current gradient in the two control periods can be written as
Δ i y ( k 1 ) = u y ( k 1 ) u x ( k 1 ) u y ( k 2 ) u x ( k 2 ) ( Δ i y ( k 2 ) Δ i x ( k 2 ) ) + Δ i x ( k 1 )
However, (11) cannot be used to update the current gradient when uy(k − 2) − ux(k − 2) = 0. In an α-axis coordinate system, seven situations may cause the stagnation effect. They are u8α = u18α, u1α = u9α = u17α, u2α = u6α, u0α = u10α = u16α, u3α = u5α, u4α = u11α = u15α, and u12α = u14α, respectively. In a β-axis coordinate system, five situations may cause the stagnation effect. They are u9β = u10β = u11β, u2β = u3β = u8β = u12β, u0β = u1β = u4β = u7β = u13β, u5β = u6β = u14β = u18β, and u15β = u16β = u17β, respectively. To eliminate the stagnation effect, (9) under the α-axis and β-axis is derived as (12) and (13), respectively. For example, when the applied voltage vector is u2, ∆i2αβ can be obtained based on (6). Then, in addition to ∆i6α (calculated based on (12)), other α-axis current gradients can be calculated based on (11). Moreover, in addition to ∆i3β, ∆i8β, and ∆i12β (calculated based on (13)), other β-axis current gradients can be calculated based on (11).
Δ i y α ( k 1 ) = Δ i x α ( k 1 )
Δ i y β ( k 1 ) = Δ i x β ( k 1 )
As a result, the stagnation effect is eliminated and the nineteen current gradients can be updated in each control period, as shown in Figure 4.

3.4. Proposed Sector Judgment Method

Conventionally, in order to find the optimal voltage vector through the cost function (4), 27 voltage vectors need to be traversed. When the redundancy state of the zero vector is ignored and the small vectors are selected as P-type small vectors or N-type small vectors according to the dc-link capacitor voltage difference, there are still 19 voltage vectors to be traversed. Since the calculation of reference voltage depends on the mathematical model, the sector judgment method based on reference voltage may cause sector judgment deviation when the model parameters are mismatched. Therefore, a sector judgment method based on the current gradient is proposed in this section.
Figure 5 shows the 19 voltage vectors and their corresponding 19 current gradients. The three-level inverter space vector coordinate system is divided into 6 large sectors and 24 small sectors. The position of the large sector where the reference current is located is judged according to the prediction currents of the medium vectors. For example, if the reference current is in large sector Ⅰ, the cost of u8 calculated by (4) is the smallest compared with the cost of u10, u12, u14, u16, and u18.
After judging the large sector, it is necessary to judge the small sector. First, the prediction currents can be calculated by (8). Then, the weighted error square ε2 of the four small sectors can be calculated by (14) and selecting the smallest ε2 corresponding sector as the target sector. Finally, there are only three voltage vectors as candidate vectors.
ε 2 = x = 1 3 ( i r e f ( k + 2 ) i g x ( k + 2 ) ) 2

3.5. Implementation Steps

Figure 6 shows the control diagram of the proposed MFPC scheme. The proposed MFPC scheme is realized to eliminate parameter dependence, the novel current gradient updating method is realized to eliminate the stagnation effect, and the sector judgment method is also realized to further reduce the computational burden over the conventional MFPC scheme. The detailed implementation steps are as follows.
  • Step I: Sample the dc-link capacitor voltage uc1(k) and uc2(k), select P-type basic voltage vectors or N-type basic voltage vectors based on uc1(k) − uc2(k) ≤ or >0.
  • Step II: Sample the output current ig(k) and calculate current gradient ∆ix(k − 1) by (6).
  • Step III: Update the remaining current gradients without stagnation effect by (11), and update the remaining current gradients with stagnation effect by (12) and (13).
  • Step IV: Calculate prediction current igx(k + 1) and igx(k + 2) by (7) and (8), respectively.
  • Step V: Judge large sectors by (4), and judge small sectors by (14).
  • Step VI: Evaluate the cost of the three voltage vectors by (4) and select the optimal vector.

4. Simulation and Experimental Evaluation

In order to verify the effectiveness of the proposed MFPC scheme, simulations in MATLAB/Simulink and experiments under the conventional MPC scheme, conventional MFPC schemes, and the proposed MFPC scheme are carried out. Figure 7 depicts the T-type three-level three-phase grid-connected inverter experimental setup. The main control chip of the inverter is DSP28335. The sampling frequency is set as 20 kHz. The inverter parameters are listed in Table 2.

4.1. Impact of Current Gradient Updating Stagnation

The proposed current gradient updating method is compared with the updating method in [20] and the updating method in [30]. Figure 8a illustrates the α-axis and β-axis current gradients when the updating method in [20] is used. In this current gradient updating method, there is a notable stagnation effect in both the current gradients ∆iα and ∆iβ because the current gradients of the applied voltage vector can be updated for the LUT; however, the remaining current gradients keep the old values. Compared to the two-level inverter system [20], the stagnation effect becomes more obvious with the increasing number of voltage vectors when the updating method [20] is used in the three-level inverter system. As shown in Figure 8b, although the updating frequency is improved, the stagnation effect still exists in the α-axis and β-axis current gradients when the updating method in [30] is used. When the updating method is converted to the proposed updating method, it can be seen that there is no stagnation effect existing in the current gradient waveforms, as shown in Figure 8b, which shows the effectiveness of the proposed updating method.

4.2. Steady-State Experimental Evaluation

Figure 9 shows the steady-state performance comparisons of the conventional MPC scheme, conventional MFPC scheme in [20], conventional MFPC scheme in [30], and the proposed MFPC scheme when model parameters match controller parameters. Based on the steady-state experimental waveforms, it can be seen that both the conventional MPC scheme, the conventional MFPC scheme in [30], and the proposed MFPC scheme can achieve tracking the reference currents and balancing the neutral point voltages. However, the neutral point voltage of the conventional MFPC scheme in [20] is affected by the current gradient stagnation effect. The harmonic spectra of the current are drawn by MATLAB/Simulink with the experimental data obtained from the oscilloscope, as shown in Figure 9.
For the conventional MPC scheme, the total harmonic distortion (THD) of phase-a output current is 3.92%. For the conventional MFPC scheme in [20], the THD of phase-a output current changes from 3.92% to 6.31% because the current performance is affected by the stagnation effect and the sampling noise effect. For the conventional MFPC scheme in [30], the THD of phase-a output current changes from 6.31% to 5.08% because the stagnation effect is improved, but it cannot be eliminated. Moreover, the current spikes caused by the stagnation effect can be observed simultaneously in Figure 9b,c. Compared with the conventional MFPC scheme in [30], the THD of phase-a output current reduces from 5.08% to 4.19% because the stagnation effect is eliminated, as shown in Figure 9d. However, the current performance of the proposed scheme is worse than that of the conventional MPC scheme because the current performance of the MFPC scheme is affected by the sampling noise.
To further verify the effectiveness of the proposed MFPC scheme, other experimental comparisons under different reference currents are carried out. The THDs of phase-a current under four control schemes are shown in Figure 10. From Figure 10, the THDs of the four control schemes are reduced with the increased reference currents. The proposed MFPC still has a similar current THD to the MPC and has a lower current THD than the MFPC in [20] and the MFPC in [30].

4.3. Experimental Evaluation under Mismatched Model Parameters

To verify the effectiveness of the proposed MFPC scheme in enhancing parameter robustness, the control performance of the proposed scheme and the conventional MPC scheme are compared in this section when the filter inductance as the model parameter is taken as different actual values from the controller values L0. It can be seen that compared with the conventional MPC scheme, the proposed scheme reduces the THD from 8.98% to 6.25% when the actual filter inductance is set as 0.05 H (i.e., 0.5L0) as shown in Figure 11. Additionally, the proposed scheme reduces the THD from 2.78% to 1.87% when the actual filter inductance is set as 0.2 H (i.e., 2L0), as shown in Figure 12. Under the above two experimental conditions, the current prediction errors of the proposed scheme are lower than that of the conventional MPC scheme. The current waveforms, the THDs, and the current prediction errors verify that the proposed scheme has stronger parameter robustness than the conventional MPC scheme.

4.4. Performance Comparison of All Schemes

In order to further demonstrate the advantages of the proposed MFPC, various performances of all schemes are compared and summarized in Table 3, including THDs, computational burden, parameter robustness, and stagnation effect. The proposed MFPC has a similar THD to MPC when model parameters are accurate and have better robustness against mismatched parameters than MPC. Though 18 current gradients in the proposed MFPC should be updated per control period, the speed of optimization is effectively reduced by the proposed sector judgment method. Hence, the proposed MFPC has a similar computational burden to MPC. For the MFPC in [20,30], although they cannot be affected by the mismatched parameters, their THDs are higher than those of the proposed MFPC because of the stagnation effect. For the MFPC in [20], it has the smallest computational burden because there is no current gradient updating exists, which leads to the largest THD. For MFPC in [30], it has the largest computational burden because there is all current gradient is updated and candidate voltage vectors are not reduced.

5. Conclusions

This paper proposes an improved MFPC scheme based on the novel current gradient updating method and the effective sector judgment method for a T-type three-level grid-tied inverter. The proposed scheme has the following salient features: First, compared to conventional MPC schemes without a weighting factor, it totally eliminates the effect of mismatched model parameters and enhances the parameter robustness, especially when the actual parameters are less than the control parameters. Then, compared to conventional MPC schemes using a weighting factor, it avoids designing the weight factor and still realizes the good control of current and neutral point voltage. Moreover, compared to conventional MFPC schemes, it eliminates the current gradient stagnation effect by the designed updating method. The THDs of the proposed scheme decrease by up to 2.12% and the current spikes caused by the long updating stagnation are avoided. Finally, the discrimination accuracy of redundant small vectors is improved by using the proposed sector judgment method based on the current gradient, and the speed of optimization is increased by 31.5%.

Author Contributions

Conceptualization, Z.Y. and T.R.; methodology, Z.Y. and Z.F.; validation, C.H. and T.R.; formal analysis, P.Z., K.L. and Z.Y.; writing—original draft preparation, Z.Y.; writing—review and editing, Z.Y., T.R., G.L. and C.H.; supervision, T.R. and C.H.; project administration, C.H. All authors have read and agreed to the published version of the manuscript.

Funding

This work is supported in part by the Outstanding youth project of Anhui Natural Science (2108085J24) and in part by the Major science and technology projects in Anhui Province (202103a05020019).

Conflicts of Interest

The authors declare that there is no conflict of interest.

References

  1. Zhang, Z.; Xu, H.; Xue, M.; Chen, Z.; Sun, T.; Kennel, R.; Hackl, C.M. Predictive control with novel virtual-flux estimation for back-to-back power converters. IEEE Trans. Ind. Electron. 2015, 62, 2823–2834. [Google Scholar] [CrossRef]
  2. Zhao, T.; Chen, D. A power adaptive control strategy for further extending the operation range of single-phase cascaded H-bridge multilevel PV inverter. IEEE Trans. Ind. Electron. 2022, 69, 1509–1520. [Google Scholar] [CrossRef]
  3. Adefarati, T.; Bansal, R.C. Integration of renewable distributed generators into the distribution system: A review. IET Renew. Power Gener. 2016, 10, 873–884. [Google Scholar] [CrossRef]
  4. Freddy, T.K.S.; Rahim, N.A.; Hew, W.P.; Che, H.S. Comparison and analysis of single-phase transformerless grid-connected PV inverters. IEEE Trans. Power Electron. 2014, 29, 5358–5369. [Google Scholar] [CrossRef]
  5. Schweizer, M.; Kolar, J.W. Design and implementation of a highly efficient three-level t-type converter for low-voltage application. IEEE Trans. Power Electron. 2013, 28, 1504–1511. [Google Scholar] [CrossRef]
  6. Schweizer, M.; Lizama, I.; Friedli, T.; Kolar, J.W. Comparison of the chip area usage of 2-level and 3-level voltage source converter topologies. In Proceedings of the IECON 2010-36th Annual Conference on IEEE Industrial Electronics Society, Glendale, AZ, USA, 7–10 November 2010; pp. 391–396. [Google Scholar]
  7. Karamanakos, P.; Geyer, T. Model Predictive Torque and Flux Control Minimizing Current Distortions. IEEE Trans. Power Electron. 2019, 34, 2007–2012. [Google Scholar] [CrossRef]
  8. Yan, L.; Wang, F.; Dou, M.; Zhang, Z.; Kennel, R.; Rodríguez, J. Active Disturbance-Rejection-Based Speed Control in Model Predictive Control for Induction Machines. IEEE Trans. Ind. Electron. 2020, 67, 2574–2584. [Google Scholar] [CrossRef]
  9. Guo, L.; Jin, N.; Gan, C.; Luo, K. Hybrid Voltage Vector Preselection-Based Model Predictive Control for Two-Level Voltage Source Inverters to Reduce the Common-Mode Voltage. IEEE Trans. Ind. Electron. 2020, 67, 4680–4691. [Google Scholar] [CrossRef]
  10. Young, H.A.; Perez, M.A.; Rodriguez, J. Analysis of Finite-Control-Set Model Predictive Current Control with Model Parameter Mismatch in a Three-Phase Inverter. IEEE Trans. Ind. Electron. 2016, 63, 3100–3107. [Google Scholar] [CrossRef]
  11. Zhang, X.; Zhang, L.; Zhang, Y. Model Predictive Current Control for PMSM Drives with Parameter Robustness Improvement. IEEE Trans. Power Electron. 2019, 34, 1645–1657. [Google Scholar] [CrossRef]
  12. Zhang, Y.; Li, B.; Liu, J. Online Inductance Identification of a PWM Rectifier under Unbalanced and Distorted Grid Voltages. IEEE Trans. Ind. Appl. 2020, 56, 3879–3888. [Google Scholar] [CrossRef]
  13. Niu, S.; Luo, Y.; Fu, W.; Zhang, X. Robust Model Predictive Control for a Three-Phase PMSM Motor with Improved Control Precision. IEEE Trans. Ind. Electron. 2021, 68, 838–849. [Google Scholar] [CrossRef]
  14. Yan, L.; Dou, M.; Hua, Z. Disturbance Compensation-Based Model Predictive Flux Control of SPMSM with Optimal Duty Cycle. IEEE J. Emerg. Sel. Top. Power Electron. 2019, 7, 1872–1882. [Google Scholar] [CrossRef]
  15. Wang, J.; Wang, F.; Wang, G.; Li, S.; Yu, L. Generalized Proportional Integral Observer Based Robust Finite Control Set Predictive Current Control for Induction Motor Systems with Time-Varying Disturbances. IEEE Trans. Ind. Inf. 2018, 14, 4159–4168. [Google Scholar] [CrossRef]
  16. Zoghdar-Moghadam-Shahrekohne, B.; Pozzi, A.; Raimondo, D.M. SOS-based Stability Region Enlargement of Bilinear Power Converters through Model Predictive Control. In Proceedings of the 2021 29th Mediterranean Conference on Control and Automation (MED), Bari, Italy, 22–25 June 2021; pp. 847–854. [Google Scholar]
  17. Zhang, Y.; Jiang, T.; Jiao, J. Model-Free Predictive Current Control of a DFIG Using an Ultra-Local Model for Grid Synchronization and Power Regulation. IEEE Tran. Energy Convers. 2020, 35, 2269–2280. [Google Scholar] [CrossRef]
  18. Jin, N.; Chen, M.; Guo, L.; Li, Y.; Chen, Y. Double-Vector Model-Free Predictive Control Method for Voltage Source Inverter With Visualization Analysis. IEEE Trans. Ind. Electron. 2022, 69, 10066–10078. [Google Scholar] [CrossRef]
  19. Rodríguez, J.; Heydari, R.; Rafiee, Z.; Young, H.A.; Flores-Bahamonde, F.; Shahparasti, M. Model-Free Predictive Current Control of a Voltage Source Inverter. IEEE Access 2020, 8, 211104–211114. [Google Scholar] [CrossRef]
  20. Lin, C.; Liu, T.; Yu, J.; Fu, L.; Hsiao, C. Model-Free Predictive Current Control for Interior Permanent-Magnet Synchronous Motor Drives Based on Current Difference Detection Technique. IEEE Trans. Ind. Electron. 2014, 61, 667–681. [Google Scholar] [CrossRef]
  21. Lin, C.; Yu, J.; Lai, Y.; Yu, H. Improved Model-Free Predictive Current Control for Synchronous Reluctance Motor Drives. IEEE Trans. Ind. Electron. 2016, 63, 3942–3953. [Google Scholar] [CrossRef]
  22. da Rù, D.; Polato, M.; Bolognani, S. Model-free predictive current control for a SynRM drive based on an effective update of measured current responses. In Proceedings of the 2017 IEEE International Symposium on Predictive Control of Electrical Drives and Power Electronics (PRECEDE), Pilsen, Czech Republic, 4–6 September 2017; pp. 119–124. [Google Scholar]
  23. Carlet, P.G.; Tinazzi, F.; Bolognani, S.; Zigliotto, M. An Effective Model-Free Predictive Current Control for Synchronous Reluctance Motor Drives. IEEE Trans. Ind. Appl. 2019, 55, 3781–3790. [Google Scholar] [CrossRef] [Green Version]
  24. Ma, C.; Li, H.; Yao, X.; Zhang, Z.; de Belie, F. An Improved Model-Free Predictive Current Control with Advanced Current Gradient Updating Mechanism. IEEE Trans. Ind. Electron. 2021, 68, 11968–11979. [Google Scholar] [CrossRef]
  25. Agustin, C.A.; Yu, J.-T.; Lin, C.-K.; Jai, J.; Lai, Y.-S. Triple-Voltage-Vector Model-Free Predictive Current Control for Four-Switch Three-Phase Inverter-Fed SPMSM Based on Discrete-Space-Vector Modulation. IEEE Access 2021, 9, 60352–60363. [Google Scholar] [CrossRef]
  26. Agustin, C.A.; Yu, J.-T.; Cheng, Y.-S.; Lin, C.-K.; Huang, H.-Q.; Lai, Y.-S. Model-Free Predictive Current Control for SynRM Drives Based on Optimized Modulation of Triple-Voltage-Vector. IEEE Access 2021, 9, 130472–130483. [Google Scholar] [CrossRef]
  27. Lin, C.-K.; Yu, J.-T.; Agustin, C.A.; Li, N.-Y. A Two-Staged Optimization Approach to Modulated Model-Free Predictive Current Control for RL-Connected Three-Phase Two-Level Four-Leg Inverters. IEEE Access 2021, 9, 147537–147548. [Google Scholar] [CrossRef]
  28. Lin, C.-K.; Agustin, C.A.; Yu, J.-T.; Cheng, Y.-S.; Chen, F.-M.; Lai, Y.-S. A Modulated Model-Free Predictive Current Control for Four-Switch Three-Phase Inverter-Fed SynRM Drive Systems. IEEE Access 2021, 9, 162984–162995. [Google Scholar] [CrossRef]
  29. Agustin, C.A.; Yu, J.-T.; Cheng, Y.-S.; Lin, C.-K.; Yi, Y.-W. A Synchronized Current Difference Updating Technique for Model-Free Predictive Current Control of PMSM Drives. IEEE Access 2021, 9, 63306–63318. [Google Scholar] [CrossRef]
  30. Yu, F.; Zhou, C.; Liu, X.; Zhu, C. Model-Free Predictive Current Control for Three-Level Inverter-Fed IPMSM With an Improved Current Difference Updating Technique. IEEE Trans. Energy Convers. 2021, 36, 3334–3343. [Google Scholar] [CrossRef]
  31. Ipoum-Ngome, P.G.; Mon-Nzongo, D.L.; Flesch, R.C.C.; Song-Manguelle, J.; Wang, M.; Jin, T. Model-Free Predictive Current Control for Multilevel Voltage Source Inverters. IEEE Trans. Ind. Electron. 2021, 68, 9984–9997. [Google Scholar] [CrossRef]
Figure 1. Topology of the T-type three-level grid-tied inverter.
Figure 1. Topology of the T-type three-level grid-tied inverter.
Energies 15 06557 g001
Figure 2. Basic voltage vectors of the three-level three-phase inverter.
Figure 2. Basic voltage vectors of the three-level three-phase inverter.
Energies 15 06557 g002
Figure 3. Control block diagram of the conventional MPC scheme.
Figure 3. Control block diagram of the conventional MPC scheme.
Energies 15 06557 g003
Figure 4. Proposed current gradient updating method.
Figure 4. Proposed current gradient updating method.
Energies 15 06557 g004
Figure 5. Big and small sectors of the three-level three-phase inverter.
Figure 5. Big and small sectors of the three-level three-phase inverter.
Energies 15 06557 g005
Figure 6. Control block diagram of the proposed MFPC scheme.
Figure 6. Control block diagram of the proposed MFPC scheme.
Energies 15 06557 g006
Figure 7. T-type three-level three-phase grid-connected inverter experimental platform.
Figure 7. T-type three-level three-phase grid-connected inverter experimental platform.
Energies 15 06557 g007
Figure 8. Current gradient comparisons under different updating methods (iref = 5A). (a) Updating method in [20]. (b) Updating method in [30]. (c) The proposed updating method.
Figure 8. Current gradient comparisons under different updating methods (iref = 5A). (a) Updating method in [20]. (b) Updating method in [30]. (c) The proposed updating method.
Energies 15 06557 g008aEnergies 15 06557 g008b
Figure 9. Experimental waveform comparisons (iref = 5A). (a) Waveforms under the conventional MPC scheme. (b) Waveforms under the conventional MFPC scheme in [20]. (c) Waveforms under the conventional MFPC scheme in [30]. (d) Waveforms under the proposed MFPC scheme.
Figure 9. Experimental waveform comparisons (iref = 5A). (a) Waveforms under the conventional MPC scheme. (b) Waveforms under the conventional MFPC scheme in [20]. (c) Waveforms under the conventional MFPC scheme in [30]. (d) Waveforms under the proposed MFPC scheme.
Energies 15 06557 g009
Figure 10. The comparison of phase-a current THDs under different reference currents.
Figure 10. The comparison of phase-a current THDs under different reference currents.
Energies 15 06557 g010
Figure 11. Experimental waveforms comparisons when L/L0 = 0.5 (iref = 5A). (a) Waveforms under the conventional MPC scheme. (b) Waveforms under the proposed MFPC scheme.
Figure 11. Experimental waveforms comparisons when L/L0 = 0.5 (iref = 5A). (a) Waveforms under the conventional MPC scheme. (b) Waveforms under the proposed MFPC scheme.
Energies 15 06557 g011
Figure 12. Experimental waveforms comparisons when L/L0 = 2 (iref = 5A). (a) Waveforms under the conventional MPC scheme. (b) Waveforms under the proposed MFPC scheme.
Figure 12. Experimental waveforms comparisons when L/L0 = 2 (iref = 5A). (a) Waveforms under the conventional MPC scheme. (b) Waveforms under the proposed MFPC scheme.
Energies 15 06557 g012
Table 1. The LUT of the T-type three-level inverter.
Table 1. The LUT of the T-type three-level inverter.
Voltage Vectoru0u1u2u3u4u5u6u7u8u9u10u11u12u13u14u15u16u17u18
Current Gradienti0i1i2i3i4i5i6i7i8i9i10i11i12i13i14i15i16i17i18
Table 2. System and control parameters.
Table 2. System and control parameters.
ParametersSymbolValues
DC-link voltageudc300 V
Peak of grid phase voltagee150 V
Grid angular frequencyωg314.16 rad/s
Control timeTs50 μs
Parasitic resistanceR0.05 Ω
Filter inductanceL010 mH
Table 3. Performance comparison of different control schemes.
Table 3. Performance comparison of different control schemes.
SchemesTHDsComputational BurdenParameter RobustnessStagnation Elimination
Conventional MPC3.92%35.9 μsNo-
Conventional MFPC in [20]6.31%31.8 μsYesNo
Conventional MFPC in [30]5.08%41.2 μsYesNo
Proposed MFPC4.19%36.2 μsYesYes
Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Share and Cite

MDPI and ACS Style

Yin, Z.; Hu, C.; Luo, K.; Rui, T.; Feng, Z.; Lu, G.; Zhang, P. A Novel Model-Free Predictive Control for T-Type Three-Level Grid-Tied Inverters. Energies 2022, 15, 6557. https://doi.org/10.3390/en15186557

AMA Style

Yin Z, Hu C, Luo K, Rui T, Feng Z, Lu G, Zhang P. A Novel Model-Free Predictive Control for T-Type Three-Level Grid-Tied Inverters. Energies. 2022; 15(18):6557. https://doi.org/10.3390/en15186557

Chicago/Turabian Style

Yin, Zheng, Cungang Hu, Kui Luo, Tao Rui, Zhuangzhuang Feng, Geye Lu, and Pinjia Zhang. 2022. "A Novel Model-Free Predictive Control for T-Type Three-Level Grid-Tied Inverters" Energies 15, no. 18: 6557. https://doi.org/10.3390/en15186557

APA Style

Yin, Z., Hu, C., Luo, K., Rui, T., Feng, Z., Lu, G., & Zhang, P. (2022). A Novel Model-Free Predictive Control for T-Type Three-Level Grid-Tied Inverters. Energies, 15(18), 6557. https://doi.org/10.3390/en15186557

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