I. INTRODUCTION
Due to the action of high-power electronic devices and the influence of reactive components, when a traditional high-power rectifier takes electricity from a power grid, a lot of harmonic currents are injected into the power system. Thus the harmonic level of the power grid is growing higher and higher on an annual basis. These harmonics pose some serious threats to other equipment drawing electricity from the power grid, such as local harmonic resonance, active loss increases, overheating and damage to shunt capacitors, metering errors, and errors in relay protection device operation. Owing to its simple circuit and easy control, the high-power diode rectifier is widely used. However, the output power cannot be controlled and with changes of the DC-side inductance, for the grid-side current harmonics, the total harmonic distortion (THD) will be 30% or above, while the THD will reach 230% or more when the inductance diminishes. Another rectifier commonly used in industry is the silicon-controlled phase-shifting rectifier bridge, whose output-side voltage can be regulated by controlling the phase angle of the thyristor. However, this introduces the problem of reactive power and a quite serious current distortion. To eliminate the interference of high-power converters on a power grid, two methods can be adopted. First, add a filter to provide pathways for the harmonic currents. This reduces the influence of harmonic currents over other electrical equipment. The other method, which is more effective, is to increase the number of rectification phases, namely increasing the number of the pulses of rectified voltage. The △-Y dual rectifier bridge (12-pulse rectifier circuit) can make the primary-side current of the power frequency transformer closer to a sine wave by superposing two winding currents on the AC-side. Thus, the grid-side harmonic current component is greatly reduced, and the harmonic frequency with the lowest order is the 11th harmonic, whose amplitude takes up only 1/11 of the amplitude of the fundamental harmonic. In addition, the THD of harmonics is less than 11%. However, the complex power frequency transformer of the circuit increases the cost and size of the entire system [1], [2].
The grid-side current or voltage is modulated into a high-frequency PWM pulse wave by a three-phase PWM rectifier. After filtering the high frequency harmonics of the grid-side current, the grid-side harmonic distortion rate can fully reach national safety standards. Fig. 1 shows a three-phase current source PWM rectifier, where the circuit is realized via controllable high-frequency switch valves with high a tolerance under high power, such as IGBT, IGCT and IECT. However, these valves cost too much money and for the latter two, only a small number of companies are able to produce them at present.
Fig. 1.Traditional 3-phase PWM current source rectifier.
The three-phase current-mode PWM rectifier with a hybrid switch is as shown in Fig. 2, where the output voltage of the circuit has the voltage drop characteristic; the grid-side current harmonic component is small; the high inductance on the output side of the circuit increases the circuit stability and safety; and the use of a thyristor provides cost advantages for the circuit. The circuit can be applied to motor drive and metal heat treatment industries [3]-[5].
Fig. 2.3-phase PWM current source rectifier with hybrid switch.
II. CIRCUIT TOPOLOGY
When compared with traditional three-phase current source PWM rectifiers, the rectifier with a hybrid switch has the following features: it uses six thyristors to replace the six IGBTs at the rectifier bridge; it uses an IGBT with the main switch tube to make a connection with rectifier bridge in series. This forces the IGBT to switch off the turn-on thyristor of the rectifier bridge. Thus, the thyristor rectifier bridge has the ability of pulse width modulation. Since the thyristor has no limitation on the latching effect, the current characteristic is far better, and the forward voltage drop is smaller than that of the controllable switch valve with the same power level, which improves the entire circuit efficiency [4], [5].
However, after the IGBT with the main switch tube is switched off, the thyristor requires a relatively long period to recover from the turn-on to the forward blocking state. This seriously restricts the working frequency of the circuit. To enhance the working frequency of the circuit for reducing the volumes of the filter elements on the AC-side and DC-side and to make it easier to filter harmonics, it is necessary to shorten the recovery time, TOFF, of the thyristor after its switching-off, or to increase the thyristor switching-off time distributed by the circuit. To shorten TOFF, it is acceptable to provide reverse voltage for the turn-on thyristor to speed up the reverse recovery process. The hybrid switch circuit after being added with the reverse voltage circuit is shown in Fig. 3. Since the reverse voltage network only needs to supply the thyristor with reverse recovery current, the switch valves for ordinary power levels can already meet the requirements for Q2. The voltage source, Umax, supplying reverse voltage is obtained through the boost transformer’s enhancing the grid-side voltage, rectification via the common diode rectifier bridge, and final filtering of the voltage-stabilizing capacitance [5]-[7].
Fig. 3.Advanced 3-phase PWM current source rectifier in addition with reverse voltage source and control system.
III. STRATEGY FOR THE CONTROL OF CURRENT SOURCE SPACE VECTORS
The three-phase current source PWM rectifier with a hybrid switch in this paper is realized by space vector control (SVPWM). Fig. 4 shows the current vectors of the three-phase current source rectifier and its axis. For SVPWM modulation, the nine current vectors in Fig. 4 are used to synthesize the required reference current vector, I* [6], [7].
Fig. 4.Current vectors of a three-phase current-mode rectifier.
In the current source space vector control method, a reference vector I* is given, as shown in Fig. 4, which can be synthesized by I1 and I6 based on the following formulas.
Where, Id is the dc side current; α is the initial phase angle of I* ; T1, T6 and T0 are the acting times of I1, I6 and I7, respectively; Ts is the switching period; and m is the modulation ratio. From formulas (1) to (4), the acting time T0 of the zero vector can be obtained. As shown in Fig. 5, I7 is distributed equally between I1 and I6, and the switching-off time provided for the thyristor is T0/2. The highest working frequency fS of the circuit is determined according to Formula (5) [7], [11].
Fig. 5.Sequence diagram of various vectors in SVPWM.
IV. OPTIMAL STRATEGY FOR CONTROL OF CURRENT SOURCE SPACE VECTORS
increase the thyristor switching-off time distributed by the control system, the specific switching process of the circuit will be analyzed as follows. As shown in Figure 4, in Sector Ⅰ, when -π/6<α<0, the grid-side capacitor voltage UA However, for the case of UA =UC, this can be avoided by setting a specific switching frequency, which can ensure that the above two cases exist when commutation. To achieve this, make sure the required recovery time of the thyristor under the condition of non-natural commutation is TOFF ; put the acting time of the remaining zero vectors before that of the vectors with natural commutation. This can ensure the normal commutation of the thyristor in the circuit, which achieves the normal conduction of the current space vectors. The minimum zero vector time of the circuit can be TOFF and the highest working frequency of the circuit is determined by Formula (6) [9]-[11]: Let the switching-off time TOFF of the thyristor be 41.67μs and the maximum modulation ratio m be 0.9. Then, according to Formula (5) of the traditional current source space vector control, the working frequency of the circuit is 1.2kHz; and according to Formula (6) of the optimal current source space vector control, the value is 2.4kHz. Under the condition of optimal space vectors, see the sequence diagram of various vectors in a sector (as shown in Fig. 6) and take Sector Ⅰ as an example. Fig. 6.Sequence diagram of vectors in Sector I of an optimal SVPWM.
References
- G. Gong, M. L. Heldwein, U. Drofenik, , J. Minibock, K. Mino, and J. W. Kolar, “Comparative evaluation of three-phase high-power-factor AC-DC converter concepts for application in future More Electric Aircraft,” IEEE Trans. Ind. Electron., Vol. 52, No. 3, 727-737, Jun. 2005. https://doi.org/10.1109/TIE.2005.843957
- M. Salo and H. Tuusa, “A vector controlled current- source PWM rectifier with a novel current damping method,” IEEE Trans. Power Electron., Vol. 15, No. 3, pp. 464-470, May 2000. https://doi.org/10.1109/63.844506
- C. Zhang, H. Gu, and B. Wang, “Mathematical model of three-phase PWM rectifier based on a novel phase and amplitude control,” in Proc. the CSEE, Vol. 23, No. 7, pp. 28-31, 2003.
- M. Malinowski, M. Jasin´ski, and M. P. Kazmierkowski, “Simple direct power control of three-phase pwm rectifier using space-vector modulation,” IEEE Trans. Ind. Electron., Vol. 51, No. 2, pp. 447-454, Apr. 2004. https://doi.org/10.1109/TIE.2004.825278
- Y. Li, H. Li, and Y. Peng, “Research on multi-level technique of three-phase current source SVPWM rectifier based on vector synthesis scheme.” in Proc. the CSEE, Vol. 27, No. 31, pp. 104-109, 2007.
- J. Dannehl, C. Wessels, and F. W. Fuchs, “Limitations of voltage-oriented PI current control of grid-connected PWM rectifiers with LCL filters,” IEEE Transactions on Industrial Electronics, Vol. 56, No. 2, pp. 380-388, Feb. 2009. https://doi.org/10.1109/TIE.2008.2008774
- B. Geethalakshmi, P. Sanjeevikumar, and P. A. Dananjayan, “PWM current source rectifier with leading power factor,” International Conference on Power Electronics, Drives and Energy Systems for Industrial Growth, 2006.
- A. Bouafia, J. P. Gaubert, and F. Krim, “Predictive direct power control of three-phase pulsewidth modulation rectifier using space-vector modulation,” IEEE Trans. Power Electron., Vol. 25, No. 1, pp. 228-236, Jan. 2010. https://doi.org/10.1109/TPEL.2009.2028731
- Y. Zhong and S. Shen, “Decoupled control and DSP implement of PWM rectifier,” in Proc. the 5th World Congress on Intelligent Controland Automation, pp. 5199-5202, 2004.
- I. Wallace, A. Bendre, J. P. Nord, G. Venkataramanan, “A unity power factor three phase PWM SCR rectifier for high power applications in the metal industry,” IEEE Trans. Ind. Appl., Vol. 38, No. 4, pp. 968-975, Jul./Aug. 2001.
- L. Jiang, Z. Cai, Z. Lü, “Research on the improved 3-phase PWM current source rectifier with hybrid switch,” Power Electronics and Motion Control Conference, 2009.
- Y. Li, Y. Peng, and H. Li, “Over-modulation technique of three-phase current source rectifier based on FPGA,” Conference on Industrial Electronics and Applications, 2007.
- F. Briz, M. W. Degner, and R. D. Lorez, “Analysis and design of current regulators using complex vectors,” IEEE Trans. Ind. Appl., Vol. 36, No. 6, pp. 817-825, May/Jun. 2000. https://doi.org/10.1109/28.845057
- C. Zhuojian, L. Jiang, R. Zhao, and H. Chen, “A hybrid three phase current source rectifier for high power application,” Power Electronics and Motion Control Conference, 2009.
- X. Jian, Z. Kai, and C. Jian, “An engineering design technique of PWM rectifier,” Adavanced Technology of Electrical Engineering and Energy, Vol. 21, No. 3, pp. 44-48, 2002.