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Advances in Power Electronics
Volume 2014 (2014), Article ID 864203, 7 pages
http://dx.doi.org/10.1155/2014/864203
Research Article

A Dynamic Model for Direct and Indirect Matrix Converters

Electrical Engineering Department, Faculty of Engineering, Ferdowsi University of Mashhad, P.O. Box 9177948974, Mashhad, Iran

Received 29 September 2013; Revised 1 March 2014; Accepted 20 March 2014; Published 8 April 2014

Academic Editor: Don Mahinda Vilathgamuwa

Copyright © 2014 Mohamad Hosseini Abardeh and Reza Ghazi. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract

The complicated modulation algorithm and the high switching frequency are two main hindrances in the analysis and simulation of matrix converters (MCs) based systems. To simplify the analysis and accelerate the simulation of MCs, a unique dynamic model is presented for the MC, which is independent of MC type (direct or indirect) and the modulation algorithm. All the input and output variables are transferred to the respective reference frames and their relations and limits are calculated. Based on the proposed equations, an equivalent circuit model is presented which can predict all the direct and indirect matrix converters dynamic and steady state behaviors without the need for small simulation time steps. Validity of the proposed model is evaluated using simulation of the precise model. Moreover, experimental results from a laboratory matrix converter setup are provided to verify the accuracy of the simulation results.

1. Introduction

The need for AC-AC power conversion is, rapidly, increasing. The power electronics converters are used for generating variable amplitude, frequency, and phase voltages and currents [1].

Matrix converter (MC) is an all-switch power converter with interesting properties such as controllable input power factor, bidirectional power flow, and high quality input and output currents. Moreover, because of the absence of the bulky DC link energy storage component, it benefits from the possibility of a compact design [2, 3]. As shown in Figure 1, there are two main types for the MC, namely, direct matrix converter (DMC) and indirect matrix converter (IMC). The application of these converters are extensive: motor drive [4, 5], FACTS devices [68], distributed generation systems [9, 10], and wind energy conversion systems [11, 12].

fig1
Figure 1: Schematic circuit of (a) direct matrix converter, and (b) indirect matrix converter.

The MC switching states are determined by modulation algorithms. Different modulation algorithms such as Alesina-Venturini (AV) method, optimum AV method, space vector modulation (SVM) [13], and duty cycle space vector (DCSV) [14, 15] have been proposed. In all cases, the modulation of the matrix converter is a complicated task and the switching frequency is usually in order of kHz (up to 45 kHz) [16]. Therefore, simulation of any MC based system is a time-consuming process, specially when the switching frequency is high. However, in dynamic and steady state studies, there is no need to consider the switching behavior of the converter regarding the study timescale. Moreover, in analytical methods for dynamic and steady state evaluation of the MC, only the knowledge of input-output relationship between voltages and currents is adequate. In these cases, by replacing the MC precise model with a dynamic model, the need for simulation and calculation of the converter switches operation is canceled out. As a consequence, the whole processes of evaluation and simulation of MC based systems become easier and much faster.

The dynamic model of power electronics converters based on methods such as averaging and principle of energy conservation is a well-known issue [17, 18]. Using these methods, different models have been presented for the matrix converters [1923]. A dynamic model in a rotating 0 frame is presented in [19]. This model is then linearized and a controller is designed on this basis. However, this model needs the knowledge of input network and the load parameters to work precisely. A dynamic model for space vector modulated MC in two independent input and output sides direct- and quadrature-axis reference frames has been developed in [20]. Although the model is independent of the source and load parameters, but its application is limited to the MCs using SVM algorithm. An equivalent circuit and a state space dynamic models for a direct matrix converter (DMC) based on the modulation matrix are proposed [21] where the input and output sides are modeled by three dependent current and voltage sources. A modeling algorithm based on the singular value decomposition (SVD) of the averaged switching matrix is presented in [22]. This method is independent of the modulation algorithm. A model based on switching state matrix averaging is presented for DMC in [23] to accelerate the fixed step simulation. It is shown that using this method the interval between simulation iterations increases from less than 250 ns up to 10 μs.

So far, the all proposed dynamic models are dependent on the converter structure (MC and IMC) and the modulation algorithm. To solve these difficulties, in this paper, a unique dynamic model for both structures of matrix converters (direct and indirect) is developed. In this model, the MC output to input voltage ratio which is independent of the modulation algorithm is used to relate the system variables. Therefore, the model besides being unique is independent of the modulation algorithm and it can be applied in various applications. In addition to the above benefits, the difficulties arising from the high frequency switches and complicated modulation algorithm are solved and the process of dynamic evaluation and simulation is greatly accelerated. The main differences between proposed model and space vector models of MC (such as the model presented in [14, 15]) are the following: in proposed model, the switching of converter is ignored since the steady state and dynamic performances are intended, and to enable control of input currents and output voltages, space vector models of the switching states are calculated by SVM; but the proposed model supposes that the modulation algorithm is working properly, and to assess the dynamic performance of the MC based systems only the input and output voltages and currents need to be calculated.

This paper begins with presentation of the matrix converter model and the equivalent circuit in Section 2. The simulation results based on the proposed model for the MC and the IMC are discussed in Section 3. In Section 4, the laboratory setup details and results are presented. Section 5 concludes the paper.

2. Matrix Converter Model

The direct and indirect matrix converter schemes are shown in Figure 1 [3, 24]. The direct matrix converters perform AC/AC power conversion in a single stage, while the indirect matrix converters do it in two stages, namely, rectification and inversion stages. The rectifier stage provides a fictitious DC link voltage with a variable average. The inverter stage synthesizes three-phase output voltages. The switching pattern can be constructed using different methods such as Venturini, space vector, and sawtooth wave modulations.

The concern of this paper is the fundamental frequency component of the MC input and output voltages and currents. Therefore, the switching effects are neglected. Based on the energy conservation rule, we have the following equation; wherein and are the input and the output active power of the MC, Transferring all the input and output voltages and currents into the respective rotating reference frames having the input and output sides angular speed, (1) leads to where subscripts “” and “” refer to the input and output quantities and subscripts “” and “” refer to direct and quadrature axis of the rotating reference frame. The input side frame is coincident with the input voltage; that is, . Equation (2) can be rewritten as follows: The MC input to output voltage ratio is where and are the output and input voltages amplitudes defined by By defining the output voltage space vector as substituting (6) in (4) yields The direct and quadrature components of can be defined as Substituting (8) in (3), we have For unity power factor at the input side, we have As the matrix converter does not always operate at unity input power factor, to have a general dynamic model, the nonzero value must be calculated. Equation (1) can be represented by the following form: where and are the input and output sides power factors and Substituting (5), (13), and (8) into (12) and after some manipulations, we obtain The input power factor is known in the modulation algorithm, but the output power factor is unknown. Substituting (2) into (12) and after some manipulations, we have Two constraints will limit the MC operation. The first one is the maximum voltage ratio 0.87 at unity power factor. The second constraint is the reduction of the maximum voltage ratio with input power factor variation according to where is the maximum voltage ratio when the input power factor is equal to . Substituting (16) into (8) and after some manipulations, we have where subscript “max” denotes the maximum value of the variable.

Figure 2 shows how measured quantities (three-phase input voltages, , and three-phase output currents, ) are used to calculate the intermediate and output variables of the model.

864203.fig.002
Figure 2: Proposed algorithm for calculation of the dynamic model variables.

3. Simulation Results

To evaluate the proposed model, direct and indirect matrix converters have been simulated using PSCAD/EMTDC software. All results are produced by setting 2 μs as the simulation time step. Figure 1 shows the benchmark system and the parameters are presented in Table 1. The input filter is RLC type and the MC switching frequency is 2.0 kHz. Space vector modulation (SVM) is used as it is compatible with digital microcontroller implementation. Inductance and capacitance of the input filter are  mH and 40 μF; therefore, the filter cut-off frequency is 795 Hz which is well below switching frequency and greater than grid frequency. The filter resistor is chosen to be 12  to increase the damping effect without adding excessive losses to the system. The MC over current protection is performed by fuses at input side of the filter which disconnect MC from grid if the input currents exceed 5 A. Inductor and resistor of load are chosen such that maximum input currents kept below 5 A. Three-phase load configuration is star. Figure 3(b) shows the input current of the precise direct and indirect matrix converter models considering the switching behavior of the converter and that of the proposed model. The voltage ratio () is varied during simulation as shown in Figure 3(a). Considering as the simulation time, the voltage ratios are 0.5 for sec, 0.86 for sec, and 0.36 for sec. The dynamic model current, as expected, does not contain the switching harmonics. However, the 50 Hz components of the precise and proposed model are close to each other and the step changes of the voltage ratio have been tracked. The same statement is also true for the output current shown in Figure 3(c). Therefore, the simulations results validate the proposed model.

tab1
Table 1: Benchmark system parameters.
fig3
Figure 3: (a) Voltage ratio, (b) input current, and (c) output current of the detailed direct and indirect matrix converter and the proposed model.

Moreover, Table 2 shows the simulation time step () for the precise and proposed model. Considering the switching frequency, should be at least ten times smaller than the switching period (50 μs). To establish a precise base for comparison, first is set equal to 2 μs. Increasing leads to acceptable results for μs for the precise model case. On the other hand, using the proposed model, can be increased up to 500 μs without losing the precision. Therefore, the simulation time can be decreased more than ten times.

tab2
Table 2: Simulation time step for the precise and proposed model.

4. Experimental Results

Attempts have been made to provide a prototype laboratory setup to test the accuracy of the proposed model. Figure 4 shows that the setup was used to implement the matrix converter. The rectifier and inverter stages, the input filter, and the microcontroller unit are specified in this figure.

864203.fig.004
Figure 4: Experimental setup.

The SVM algorithm is implemented using an ARM based microcontroller (SAM7X256 from ATMEL) which has 55 MHz clock frequency. The development tool used for the ARM is Keil Vision version 4.0. The MCU generates 12 gate pulses for the rectifier and inverter stages. Two ADC channels are used to read sensors which measure the matrix converter input voltages. Two line voltages are measured by AD202 isolation amplifier (from Analog Device) and the third line voltage is calculated considering a balanced three-phase source. The MC is implemented using 18 IGBT switches provided by Fuji electric (1MBH30D). The switching frequency () is 2 kHz. A RLC filter ( Ω,  mH, and C ) is connected to the MC input side to reduce the switching harmonics. The load is a three-phase balanced RL ( Ω and  mH) with star configuration. The input grid and output voltage frequencies are and Hz.

Figure 5 shows the proposed matrix converter model and the experimental input and output currents. The voltage ratio is changed from 0.5 to 0.79 at sec and from 0.79 to at sec. The input side currents (Figure 5(a)) of the experimental setup and that of the proposed model have a good agreement. The model can predict the MC input current dynamic variations precisely. However, because of the parasitic resistance of the input filter inductor and the switching losses, the actual current is smaller than the dynamic model current.

fig5
Figure 5: (a) Input, and (b) output current of the proposed model and the experimental setup.

The output current of the actual MC and the proposed model is shown in Figure 5(b). The model does not generate the switching frequency components. Moreover, the actual output current is smaller than the model current because of the voltage drop over switches, the conduction resistor of the switches, and the voltage drop over the input filter parasitic resistor.

Figure 6 shows how the output current of the model and the actual MC will vary following a step change in the output frequency. At 0.1 sec, the output frequency is increased from 30 to 60 Hz. The model output current tracks the actual MC current precisely.

864203.fig.006
Figure 6: MC output current.

In another application of the proposed model, a squirrel cage induction motor (SCIM) driven by a MC is tested. The motor parameters are presented in Table 3. A 2.1 kW wound rotor induction motor (WRIM) is used as a dynamic load. The motor voltage is decreased from 200 V to 110 V during 0.4 sec. One phase of the motor current is shown in Figure 7. The proposed model is used in simulations. Comparison of the simulation and experimental results shows that the dynamic model can predict the MC dynamic operation with a good precision. Moreover, motor speed in experimental test is depicted in Figure 8. The speed is decreased because of the voltage drop.

tab3
Table 3: SCIM parameters.
864203.fig.007
Figure 7: SCIM current.
864203.fig.008
Figure 8: SCIM speed.

5. Conclusion

Owing to the complicated modulation algorithm and the high switching frequency (up to tens of kHz), analysis and simulation of the MC based systems become a hard and time-consuming task. Therefore, based on the dynamic equations of the MC, an equivalent circuit model has been developed to simplify the MC analysis and accelerate the simulations. The model is independent of the MC type (direct or indirect) and the modulation algorithm. Simulation and experimental results have shown the validity and precision of the proposed model to predict the MC fundamental frequency behavior.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

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