基于实验数据和有限元法的电磁执行器鲁棒H∞力控制

R. Tahmasebi, H. Alizadeh, Saman Rahimi, B. Boulet
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引用次数: 13

摘要

本文研究了电磁执行器的鲁棒力控制问题。这种控制问题是研究手动自动变速器电动汽车换挡控制的一个重要问题。实验系统辨识与有限元法(FEM)是本文考虑的电磁作动器动态行为和系统不确定性建模的方法。通过实验系统辨识,建立了执行器的动力学模型,并建立了电磁力与电流和气隙的非线性代数模型。利用磁性材料的特性和作动器的几何形状,利用Magnet®- Infolytica软件进行有限元分析,获得公称系统的动力学特性,并验证系统辨识结果。考虑驱动系统所涉及的物理参数的固有不确定性以及测量误差,对电磁阀系统进行不确定性分析,得到电磁阀系统的动态不确定性模型。考虑到该驱动器在换挡过程中的应用,针对期望的换挡质量定义了闭环性能目标。同时了解系统的标称模型和不确定性模型,设计了H∞鲁棒控制器。对所得到的鲁棒闭环控制系统的性能进行了标称和摄动系统的检验,并证明其满足目标。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Robust H∞ force control of a solenoid actuator using experimental data and finite element method
In this paper, the robust force control of a solenoid actuator is studied. Such control problem is of interest in the study of gear shifting control in electric vehicles (EVs) equipped with an automated manual transmission (AMT). Experimental system identification together with the finite element method (FEM) is the approach considered in this paper to model the dynamic behavior of the solenoid actuator as well as the system uncertainties. Using experimental system identification, a dynamic model of the actuator is obtained and a nonlinear algebraic model of the electromagnetic force versus current and air gap is proposed. Using the properties of the magnetic materials and the geometry of the actuator, an FEM analysis is performed using Magnet® - Infolytica software - to obtain the dynamics of the nominal system and verify the system identification result. Considering the inherent uncertainty of the physical parameter involved in the actuation system as well as the measurement errors, an uncertainty analysis is performed to obtain the dynamic uncertainty model of the solenoid system. Moreover, considering the application of such actuator in the gear shifting process, the closed-loop performance objectives are defined with respect to the desired gear shifting quality. Knowing both the nominal system model and the uncertainty model, an H∞ robust controller is designed. The performance of the resulting robust closed-loop control system is examined for the nominal and perturbed systems and is shown to satisfy the objectives.
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