电子科技 ›› 2024, Vol. 37 ›› Issue (3): 34-43.doi: 10.16180/j.cnki.issn1007-7820.2024.03.005
袁庆庆1, 吴瑞麒1, 马婷2, 谢晓彤1
收稿日期:
2022-10-25
出版日期:
2024-03-15
发布日期:
2024-03-11
作者简介:
袁庆庆(1987-),女,博士,副教授。研究方向:高性能电机控制。基金资助:
YUAN Qingqing1, WU Ruiqi1, MA Ting2, XIE Xiaotong1
Received:
2022-10-25
Online:
2024-03-15
Published:
2024-03-11
Supported by:
摘要:
全桥逆变器电机驱动或称开绕组结构虽然兼具相间电气隔离、容错性能好及器件开关频率低等优点,但存在逆变器输出电压矢量多、冗余严重且控制约束等问题。文中以共直流母线供电的六相全桥逆变器驱动六相永磁同步电机为研究对象,提出了一种基于二级矢量优化的简化模型预测电流控制算法,在实现电机定子基波电流有效跟踪控制的同时有效抑制了定子电流的谐波及零序分量。文中基于矢量空间解耦理论对六相全桥逆变器的输出电压矢量进行了分层分析,以定子基波电流控制、谐波及零序电流抑制为准则对逆变器输出的729个电压矢量进行二级优化,得到候选的12个电压矢量,以此为基础设计了模型预测电流控制算法。实验结果表明,该简化模型预测电流控制方法具有良好的动静态性能,能在基波电流控制的同时有效抑制谐波及零序电流分量,可为多相电机驱动系统研究提供一定的理论支撑。
中图分类号:
袁庆庆, 吴瑞麒, 马婷, 谢晓彤. 六相全桥逆变器驱动PMSM的简化模型预测电流控制[J]. 电子科技, 2024, 37(3): 34-43.
YUAN Qingqing, WU Ruiqi, MA Ting, XIE Xiaotong. Simplified Model Predictive Current Control for the Six-Phase Full-Bridge Inverter Fed PMSM Drive[J]. Electronic Science and Technology, 2024, 37(3): 34-43.
表1
αβ子空间上的矢量分布(假设Vdc/3=1 V)"
电压幅值 | 矢量数量 | 电压幅值 | 矢量数量 |
---|---|---|---|
0 | 9 | 1.931 9 | 48 |
0.267 9 | 12 | 2.000 0 | 36 |
0.517 6 | 48 | 2.236 1 | 48 |
0.732 1 | 24 | 2.394 2 | 48 |
0.896 6 | 12 | 2.449 5 | 12 |
1.000 0 | 72 | 2.732 1 | 24 |
1.035 3 | 12 | 2.828 4 | 12 |
1.239 3 | 48 | 2.909 3 | 48 |
1.414 2 | 48 | 3.234 8 | 24 |
1.506 0 | 48 | 3.346 1 | 12 |
1.732 1 | 36 | 3.732 1 | 12 |
1.880 4 | 24 | 3.863 7 | 12 |
表2
αβ子平面和xy 子平面上所有729个电压矢量的映射关系(假设Vdc/3=1 V)"
层数 | 矢量幅值 | 幅值差 | 矢量数 | |
---|---|---|---|---|
αβ | xy | |||
1 | 0.000 0 | 0.000 0 | 0.000 0 | 9 |
2 | 0.267 9 | 3.732 1 | -3.464 1 | 12 |
3 | 0.517 6 | 1.931 9 | -1.414 2 | 48 |
4 | 0.732 1 | 2.732 1 | -2.000 0 | 24 |
5 | 0.896 6 | 3.346 1 | -2.449 5 | 12 |
6 | 1.000 0 | 1.000 0 | 0.000 0 | 72 |
7 | 1.035 3 | 3.863 7 | -2.828 4 | 12 |
8 | 1.239 3 | 2.909 3 | -1.670 0 | 48 |
9 | 1.414 2 | 1.414 2 | 0.000 0 | 48 |
10 | 1.506 0 | 2.394 2 | -0.888 2 | 48 |
11 | 1.732 1 | 1.732 1 | 0.000 0 | 36 |
12 | 1.880 4 | 3.234 8 | -1.354 4 | 24 |
13 | 1.931 9 | 0.517 6 | 1.414 2 | 48 |
14 | 2.000 0 | 2.000 0 | 0.000 0 | 36 |
15 | 2.236 1 | 2.236 1 | 0.000 0 | 48 |
16 | 2.394 2 | 1.506 0 | 0.888 2 | 48 |
17 | 2.449 5 | 2.449 5 | 0.000 0 | 12 |
18 | 2.732 1 | 0.732 1 | 2.000 0 | 24 |
19 | 2.828 4 | 2.828 4 | 0.000 0 | 12 |
20 | 2.909 3 | 1.239 3 | 1.670 0 | 48 |
21 | 3.234 8 | 1.880 4 | 1.354 4 | 24 |
22 | 3.346 1 | 0.896 6 | 2.449 5 | 12 |
23 | 3.732 1 | 0.267 9 | 3.464 1 | 12 |
24 | 3.863 7 | 1.035 3 | 2.828 4 | 12 |
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