I. INTRODUCTION
In recent years, Saleh has proposed and developed the wavelet modulation techniques on different two-level converters [1]-[5]. The wavelet modulation technique is based on establishing a non-dyadic type multi resolution analysis (MRA), which is required to support a non-uniform recurrent sampling–reconstruction process. The merits of this approach includes simpler realization by digital algorithm, higher magnitudes of the fundamental output voltage, and lower harmonic contents better than other types of modulation techniques. In [1] and [2], the manner of implementation of a wavelet modulation technique for single-phase voltage source inverters was proposed. The manner of implementation of a wavelet modulation technique for three-phase voltage-source six-pulse inverters was proposed in [3] and [4]. In [5], the manner of implementation of a wavelet modulation technique for AC–DC converters was proposed. Hence, the present research on the WPWM technique focuses on the two-level inverter.
Compared with the two-level inverter, the three-level inverter is a new type of high-voltage large capacity power converter with advantages of having improved voltage waveform on the AC side, smaller filter size, lower electromagnetic interference, and lower acoustic noise [6]. Therefore, three-level inverter options are attracting greater attention in the fields of the grid interconnection, new energy, fuel electromagnetic [7], [8]. Because of the wide application of three-level inverters, the study of its control strategy has been increasingly highlighted [9]-[15]. One of commonly used control strategies is sinusoidal pulse width modulation (SPWM). The SPWM technique for two-level inverters only needs a modulating signal and a carrier signal, but the conventional SPWM technique for three-level inverters needs a modulating signal, two carrier signals, and a square signal. Thus, directly applying the WPWM technique to three-level inverters is impossible because the WPWM technique to two-level inverters can only generate two unipolar-controlled signals or two bipolar-controlled signals.
Thus, this paper presents the development and performance testing of the WPWM technique for single-phase three-level inverters. The single-phase three-level inverter with SPWM technique is reviewed in Section II. The single-phase three-level inverter with WPWM technique is proposed in Section III. The analysis of the WPWM technique for the single-phase three-level inverter is provided in Section IV. The experimental results are obtained in Section V. Conclusions are given in Section VI.
II. SINGLE-PHASE THREE-LEVEL INVERTER WITH SPWM TECHNIQUE
Fig. 1 shows the circuit schematic of an asymmetric single-phase three-level inverter [17], [18]. The circuit is composed of a two-level bridge and a three-level bridge. C1 and C2 are the DC side filter capacitor. Ud is the DC voltage source. When Ud=E, Uao has three levels, i.e., +E/2, 0, and –E/2, and Ubo has two levels: +E/2, and –E/2, which, in total, gives output voltage Uab five levels. The operation states of single-phase three-level inverter are listed in TABLE I.
Fig. 1.Scheme of the single-phase three-level inverter.
TABLE IOPERATION STATES OF THE SINGLE-PHASE THREE-LEVEL INVERTER
A conventional SPWM scheme is shown in Fig. 2 [18], which has a reference rectified sine wave (Vref) and two carrier signals (vtri1 and vtri2). The comparison result of Vref and vtri1 is the control signal of A1; the comparison result of Vref and vtri2 is the control signal of B1; the comparison result of Vref and zero is the control signal of C1. Then, the control signals for switches S1–S6 can be derived by A1, B1, and C1, as shown in Fig. 3, where S1 = A1 and ;
Fig. 2.SPWM operation principle of the three-level inverter.
Fig. 3.Logic control scheme for switches S1–S6.
III. WPWM TECHNIQUE FOR SINGLE-PHASE THREE-LEVEL INVERTER
A. Principle of the WPWM Technique
The WPWM technique is based on sampling–reconstructing a reference-modulating signal in a non-uniform recurrent manner using sets sampling and synthesis basis functions [1,2]. These sampling basis functions are generated as dilated and translated versions of the scale-based linearly-combined scaling function φ(j,k)(t) . Furthermore, synthesis basis functions are generated as dilated and translated versions of the scale-based linearly combined synthesis scaling function The scale-based linearly-combined scaling function is defined at scale j as
and φ(j,k)(t)=φ(2j t-k), where j=0, 1, 2, 3, … and ϕH(t) is the Harr scaling function that is given by
Moreover, synthesis scaling function associated with φ(t) can be defined as
Using these two dual scaling functions, a continuous-time signal xc(t) can be expanded as
where j, k ∈ Z, where Z is the set of integer numbers. Such form of signal processing suggests that a continuous-time signal
The work on [10] proved that the switching pulses for the inverter can be generated by using dilated and shifted versions of synthesis scaling function When each cycle of xc(t) is divided by a finite number of sample groups D, the length of the time interval of the sample group [td1, td2] changes as scale j changes, where
In addition, based on the the procedure on how to implement the WPWM technique given in [1], the flowchart for WPWM can be shown as Fig. 4 [16], where Tm is the period of the reference sine wave.
Fig. 4Flowchart of the WPWM technique implementation.
B. WPWM Strategy for the Single-Phase Three-Level Inverter
According to the above flowchart of WPWM, once Tm, j0 and D are given, the time points (td1 and td2) of each sample group can be calculated, and the driving pulses can be generated by the time points in each sample group, which can be integrated into two unipolar-controlled signals (W1and W2). However, the signals (W1and W2) cannot be used to control the switches of single-phase three-level inverter directly. Thus, based on Figs. 2 and 3, the WPWM operation principle for the three-level inverter can be shown as Fig. 5. W1and W2 are generated according to the flowchart of the WPWM technique shown in Fig. 4. Pulse P1 has a half-cycle symmetry property, its frequency is the double of reference sine wave, and its pulse width can be varied to adjust the distribution of the output voltage levels, which will be discussed in detail in the following. Pulse C1 is a square signal, and its frequency is the same as the reference sine wave. Then, the control signals for switches S1–S6 can be derived by the specific logic relationship among W1, W2, P1, and C1, as shown in Fig. 6, where
and
Fig. 5.WPWM operation principle of three-level inverter.
Fig. 6.Logic control scheme for the switches S1~S6 with WPWM technique.
Moreover, Fig. 6 shows that the WPWM control strategy for the single-phase three-level inverter can be implemented simply by a digital algorithm.
IV. ANALYSIS OF THE WPWM TECHNIQUE FOR THE SINGLE-PHASE THREE-LEVEL INVERTER
To verify the control strategy of the WPWM technique for the single-phase three-level inverter, a MATLAB/SIMULINK model is built and simulation is made by selecting D=30, fm=50 Hz (fm is the frequency of the reference sine wave), j0=0, the pulse width of P1 is 50%, the simulation results of signals W1, W2, W3, P1, C1, and S1–S6 can be obtained, as shown in Fig. 7. When input voltage Ud=50 V, output voltage Uab is shown in Fig. 8.
Fig. 7.Signals of W1, W2, W3, P1, C1, and S1–S6 at D=30, fm=50 Hz, j0=0.
Fig. 8.Output voltage Uab.
According to the control strategy of the WPWM technique for the single-phase three-level inverter, the width and position of the pulses (W1and W2) generated by the WPWM technique are determined when D and j0 are given, and C1 is a determined square wave when the frequency of the reference sine wave is given. Therefore, the only way of changing the control signals for switches S1–S6 is by adjusting the pulse width of P1, the distribution of the output voltage levels is affected.
To analyze the effects of pulse P1 on the distribution of the output voltage levels, this study selects D=30, fm=50 Hz, j0=0, and input voltage Ud=50 V as a sample object to be simulated based on the MATLAB/SIMULINK model of a single-phase three-level inverter, as shown in Fig. 2. The pulse width of P1 is chosen in the range of 10%–90%. The simulation results of the total harmonic distortion (THD) and the amplitude of fundamental voltage V1 for output voltage Uab are shown in Figs. 9 and 10, respectively. Fig. 9 shows that the THD is smallest when the pulse width of P1 is about 62%. Fig. 10 shows that V1 increases as the pulse width of P1 increases, and V1 can be larger than the input voltage when the pulse width is larger than 50%.
Fig. 9.THD of Uab vs. the pulse width of P1.
Fig. 10.V1of Uab vs. the pulse width of P1.
V. EXPERIMENTAL RESULTS
To verify the analysis of the WPWM technique for the single-phase three-level inverter, the algorithm of the WPWM technique is implemented by using DSP (TMS320LF2812), and the input voltage of the single-phase three-level inverter is 0V Vdc=50V , MOSFET IRFPE40 is selected as switch, TLP250 is used as driver, and pure resistance R = 50 Ω is used as the load. A photograph of the experimental setup is shown in Fig. 11. Note that the value of the THD is tested by Fluke Norma 5000 Power Analyzer.
Fig. 11.Photograph of the experimental setup.
First, the experiments have been performed by choosing fm=50 Hz, j0=0, D=30, and the pulse width of P1=40%, 50%, 60%, 62%, 63%, 70%, 80%, and 90%. The experimental results are shown in Fig. 12. Fig. 12(a) shows that the THD is smallest when the pulse width of P1 is about 62%, and Fig. 12(b) shows that V1 increases as the pulse width of P1 increases, which are consistent with the simulation results shown in Figs. 9 and 10.
Fig. 12.Experimental results of the THD and V1vs. the pulse width of P1 at j0=0, fm=50 Hz, D=30.
Second, the experiments have been performed by choosing fm=50 Hz, j0=0, the pulse width of P1 =62%, and D=20, 30, 40. The experimental results are shown in Figs. 13(a)-13(c). Fig. 13 shows that using the WPWM technique to control the single-phase three-level inverter is effective.
Fig. 13.Output voltage Uab and its spectrum of the single-phase three-level inverter by WPWM.
Finally, to validate the performance of the single-phase three-level inverter with the WPWM technique, this paper compares the WPWM with conventional SPWM, as shown in Fig. 2. The algorithm of the conventional SPWM is implemented by using DSP (TMS320LF2812), and the experiments have been performed by choosing fm=50 Hz, m=1.0 (m denotes the modulation index), the switching frequency fs =1 kHz (D=20), fs =1.5 kHz (D=30), and fs =2 kHz (D=40). The experimental results are shown in Fig. 14(a), (b), (c) respectively.
Fig. 14.Output voltage Uab and its spectrum of the single-phase three-level inverter by the SPWM.
The compared results between WPWM and SPWM from Figs. 13 and 14 are listed in TABLE II. From TABLE II, it can be concluded that (1) WPWM can get higher magnitudes of the fundamental component than SPWM; (2) WPWM technique can get smaller THD and more disperser spectrum than SPWM.
TABLE IICOMPARISON OF RESULTS BETWEEN WPWM AND SPWM FROM FIGS. 13 AND 14
VI. CONCLUSION
This study has developed the WPWM technique for single-phase three-level inverters. The design of the parameter for the WPWM is obtained by analyzing the magnitudes of the fundamental frequency component and harmonic distortion of its output voltage. The simulation and experimental results have shown that the proposed WPWM for the three-level inverter can obtain higher magnitudes of the output fundamental frequency component, lower THD, and simpler digital implementation than the SPWM, which will promote the application of WPWM technique in power electronics converters.
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