Model-based synthesis of nonlinear PI and PID controllers
- 格式:pdf
- 大小:248.89 KB
- 文档页数:14
2023年第47卷第11期Journal of Mechanical Transmission基于MPC的麦克纳姆轮移动平台轨迹跟踪控制黄晓宇1,2孙勇智1,2李津蓉1,2王翼挺1,2杨颀伟1,2(1 浙江科技学院自动化与电气工程学院,浙江杭州310023)(2 浙江省机器人产业学院,浙江杭州310023)摘要针对麦克纳姆轮全向移动平台轨迹跟踪控制问题,提出了一种模型预测控制(Model Pre⁃dictive Control,MPC)和微分先行比例-积分-微分(Proportional plus Integral plus Derivative,PID)协同的双闭环控制策略。
基于麦克纳姆轮运动学特点,设计了位姿控制环和速度控制环;在位姿控制环建立麦克纳姆轮底盘的线性误差模型,设计二次型目标函数,将路径跟随问题转化为对非线性模型的预测控制;在速度控制环引入微分先行PID控制器,避免输入量频繁的阶跃变化对系统产生高频干扰,加快麦克纳姆轮的角速度收敛,增强了系统稳定性。
仿真实验表明,设计的控制器在收敛速度、跟踪精度方面均高于常见的轨迹跟踪器,对麦克纳姆轮移动平台的控制具有良好的鲁棒性。
关键词麦克纳姆轮轨迹跟踪线性误差模型模型预测控制微分先行PIDTrajectory Tracking Control of Mecanum Wheels Mobile Platform Based on MPC Huang Xiaoyu1,2Sun Yongzhi1,2Li Jinrong1,2Wang Yiting1,2Yang Qiwei1,2(1 School of Automation and Electrical Engineering, Zhejiang University of Science and Technology, Hangzhou 310023, China)(2 Key Institute of Robotics of Zhejiang Province, Hangzhou 310023, China)Abstract For the trajectory tracking control problem of the omnidirectional mobile platform of Mecanum wheels, a strategy of double closed-loop control with model predictive control (MPC) and differential forward proportional plus integral plus derivative (PID) is proposed. The attitude control loop and velocity control loop are designed based on the kinematics characteristics of Mecanum wheels. The linear error model of the Mecanum wheels chassis is established by the attitude control loop, the quadratic objective function is designed, and the problem of path following is transformed into predictive control for the nonlinear model. In the velocity control loop, the differential forward PID controller is used to avoid the high-frequency disturbance to the system caused by frequent step changes of the input quantity, accelerate the convergence of the angular velocity of the Mecanum wheels, and enhance the stability of the system. Simulation experiments demonstrate that the controller designed in this study has better convergence speed and tracking accuracy than the commonly used trajectory algorithm, and it can provide good robustness to control the mobile platform of Mecanum wheels.Key words Mecanum wheel Trajectory tracking Linear error model Model predictive control Dif⁃ferential forward PID0 引言随着计算机的应用和传感技术的发展,移动机器人技术在智能制造、工业物流等领域得到广泛应用[1-2]。
MDA盐水处理系统的废料最小化岳金彩,杨霞,程华农,郑世清(青岛科技大学计算机与化工研究所,山东青岛266042)摘要:MDA生产过程中产生大量含苯胺、MDA废盐水,需进行萃取、汽提处理,以回收大部分有用组分。
本文建立了MDA盐水处理系统废料最小化问题的严格数学模型,此模型属于多目标混合整数非线性规划(MOMINLP),求解比较困难。
运用基于多目标遗传算法的过程综合三层次解算策略对MDA盐水处理系统的废料最小化问题进行求解,得到了非劣解曲线。
非劣解曲线由三部分组成,分别代表了三种萃取流程。
对影响利润目标的价格系数进行灵敏度分析,表明回收产品胺的价格变动对利润影响最大,蒸汽价格其次,而设备费用最小。
由于使用了严格过程模型,本文研究结果能为工程设计提供依据。
关键词:MDA;废料最小化;多目标遗传算法;Aspen Plus中图分类号:TQ021.8文献标识码:A文章编号:Waste minimization of MDA brine treatment processYUE Jincai,YANG Xia,CHENG Huanong,ZHENG Shiqing(Research Center for Computer and Chemical Engineering, Qingdao University of Science and Technology,Qingdao266042,Shandong,China)Abstract:A great amount of brine containing aniline and MDA is produced in MDA production process,which is discharged after extracting and steam-stripping in order to recover useful component.The rigid model of waste minimization of brine treatment process is proposed.The model is described as a multi-objective mixed-integer nonlinear programming(MOMINLP)which is difficult to solve.The model of the waste minimization is solved by using a strategy called three-layer solution algorithm for multi-objective synthesis based on MOGA.The non-inferior set which includs three sections is attained.Sensitivity analysis is used to study the influence of price factors on profit objective and the sequence of influence degree is amine price,steam price and the equipment price.Due to the rigid process model,the results of this paper can be used to design the industry process.Key words:MDA;Waste minimization;MOGA;Aspen plus二苯基甲烷二胺(简称MDA)是一种重要的化工中间体。
单一的神经网络PI控制高可靠性直线电机磁浮摘要:本文论述了一种可以改善系统可靠性的新型线性鼠笼电机(linear induction motor, LIM)从LIM的标准电路方程考虑动力学终端效应,当制动特性同时作为影响力时,可以建立包含有大的补偿终端效应的等效电路模型。
等效电路模型可以用作LIM的二次磁场定向控制。
同时讨论了单神经网路PI单元作为LIM的辅助驱动效果,驱动控制的数学模型的有效性通过模拟实验被证实。
关键字:线性鼠笼电机(LIM),磁场定向控制,终端效应前言线性鼠笼电机是在低速磁浮系统中作为耐热系统,来驱动车辆。
LIM 之所以有终端效应取决于它独特的装置。
由动力学终端效应产生的涡流动力导致了线性电机的额外损失,从而减少了推动力。
当矢量控制策略应用于LIM时,就必须考虑终端效应的影响,并且建立更精确的数学模型来完善控制系统的整体性能。
在本文中,讨论了在考虑终端效应很大时LIM的电路方程,推导出了LIM的计算模型。
智能控制方法被用来解决人力所难以操作的问题。
而单神经PI控制单元之所以能被用于LIM的辅助驱动是由于它简单的构造。
模拟实验已经证实了这些模型在改善整体性能上的有效性和可靠性。
考虑了终端效应的LIM的电路方程在一个长的二级类型的LIM中,和一级不同的是在二级类型中连续更换了新材料,这种新材料倾向于抵制渗透通量的突然增加,且只允许空间间隙中渗透密度的逐渐积聚。
在二级板块的进口端和出口端,因为磁通量的突然转变,会产生涡流,这种感应电流可以避免气隙磁场的突然改变。
考虑到动力学终端效应,线性电机的有效长度假设为l,二级参数转化为一级参数,在二级核心的进口端,涡流迅速增加,增加速率可以由下式计算:T1 = L r1 / R r式中:L r1——由二级转化为一级的渗漏电感系数;R r ——由二级转化为一级的等效电阻。
因为T1 = L r1 / R r的值很小,故可以忽略。
二级涡流可以迅速的达到一级励磁电流,而一级电流的涡流阶段则相反。
MITResearch in nano- and micro- scale technologies is in the departments of Material Sci. and Eng. And Computer Sci. or Chemical Eng.MIT’s major micro and nano centers are MTL(Microsystem Technology Laboratories) which provide microelectronics fabrication lab/research/index.html.MTL is home to several research centers, including:∙The Center for Integrated Circuits and Systems (CICS) serves to promote closer technical relation between MIT's Microsystems Technology Lab's (MTL) research and industry, initiate and fund new research in integrated circuits and systems, produce more students skilled in the same area, address important research issues relevant to industry, and solicit ideas for new research from industry.∙The Intelligent Transportation Research Center (ITRC) focuses on the key Intelligent Transportation Systems (ITS) technologies, including an integrated network of transportation information, automatic crash & incident detection, notification and response, advanced crashavoidance technology, advanced transportation monitoring and management, etc., in order toimprove the safety, security, efficiency, mobile access, and environment. There are two emphasis for research conduced in the center: the integration of component technology research andsystem design research, and the integration of technical possibilities and social needs.∙MEMS@MIT is a collection of faculty/staff/students working in the broad area of a Micro/nano systems and MEMS. This center was created to serve as a forum for collectingintellectually-synergistic but organizationally diverse groups of researchers at MIT. In addition, we have organized an industrial interaction mechanism to catalyze the transfer of knowledge to the larger MEMS community.The research:Chemical/Mechanical/Optical MEMS1. A MEMS Electrometer for Gas Sensing2. A Single-Gated CNT Field-Ionizer Array with Open Architecture3. A MEMS Quadrupole that Uses a Meso-scaled DRIE-patterned Spring Assembly System4. Digital Holographic Imaging of Micro-structured and Biological Objects5. Multi-Axis Electromagnetic Moving-Coil Microactuator6. Multiphase Transport Phenomena in Microfluidic Systems7. Microfluidic Synthesis and Surface Engineering of Colloidal Nanoparticles8. Microreactor Enabled Multistep Chemical Synthesis9. Integrated Microreactor System10. Crystallization in Microfluidic Systems11. Microreactors for Synthesis of Quantum Dots12. A Large Strain, Arrayable Piezoelectric Microcellular Actuator13. MEMS Pressure-sensor Arrays for Passive Underwater Navigation14. A Low Contact Resistance MEMS-Relay15. "Fast Three-Dimensional Electrokinetic Pumps for Microfluidics16. Carbon Nanotube - CMOS Chemical Sensor Integration17. An Energy Efficient Transceiver for Wireless Micro-Sensor Applications18. Combinatorial Sensing Arrays of Phthalocyanine-based Field-effect Transistors19. Nanoelectromechanical Switches and Memories20. Integrated Carbon Nanotube Sensors21. Organic Photovoltaics with External Antennas22. Integrated Optical-wavelength-dependent Switching and Tuning by Use of Titanium Nitride (TiN)MEMS Technology23. Four Dimensional Volume Holographic Imaging with Natural Illumination24. White Light QD-LEDs25. Organic Optoelectronic Devices Printed by the Molecular Jet Printe26. Design and Measurement of Thermo-optics on SiliconBioMEMS1. A Microfabricated Platform for Investigating Multicellular Organization in 3-D Microenvironments2. Microfluidic Hepatocyte Bioreactor3. Micromechanical Control of Cell-Cell Interaction4. A MEMS Drug Delivery Device for the Prevention of Hemorrhagic Shock5. Multiwell Cell Culture Plate Format with Integrated Microfluidic Perfusion System6. Characterization of Nanofilter Arrays for Biomolecule Separation7. Patterned Periodic Potential-energy Landscape for Fast Continuous-flow BiomoleculeSeparation8. Continuous-flow pI-based Sorting of Proteins and Peptides in a Microfluidic Chip Using DiffusionPotential9. Cell Stimulation, Lysis, and Separation in Microdevices10. Polymer-based Microbioreactors for High Throughput Bioprocessing11. Micro-fluidic Bioreactors for Studying Cell-Matrix Interactions12. A Nanoscanning Platform for Biological Assays13. Label-free Microelectronic PCR Quantification14. Vacuum-Packaged Suspended Microchannel Resonant Mass Sensor for BiomolecularDetection15. Microbial Growth in Parallel Integrated Bioreactor Arrays16. BioMEMS for Control of the Stem-cell Microenvironment17. Microfluidic/Dielectrophoretic Approaches to Selective Microorganism Concentration18. Microfabricated Approaches for Sorting Cells Using Complex Phenotypes19. A Continuous, Conductivity-Specific Micro-organism Separator20. Polymer Waveguides for Integrated BiosensorsEnabling Technology1. A Double-gated CNF Tip Array for Electron-impact Ionization and Field Ionization2. A Double-gated Silicon Tip, Electron-Impact Ionization Array3. A Single-Gated CNT Field-Ionizer Array with Open Architecture4. Aligning and Latching Nano-structured Membranes in 3D Micro-Structures5. Characterization and Modeling of Non-uniformities in DRIE6. Understanding Uniformity and Manufacturability in MEMS Embossing7. Atomic Force Microscopy with Inherent Disturbance Suppression for Nanostructure Imaging8. Vacuum-Sealing Technologies for Micro-chemical Reactors9. Direct Patterning of Organic Materials and Metals Using Micromachined Printheads10. MEMS Vacuum Pump11. Rapid and Shape-Controlled Growth of Aligned Carbon Nanotube Structures12. Prediction of Variation in Advanced Process Technology Nodes13. Parameterized Model Order Reduction of Nonlinear Circuits and MEMS14. Development of Specialized Basis Functions and Efficient Substrate Integration Techniques forElectromagnetic Analysis of Interconnect and RF Inductors15. A Quasi-convex Optimization Approach to Parameterized Model-order Reduction16. Amorphous Zinc-Oxide-Based Thin-film Transistors17. Magnetic Rings for Memory and Logic Devices18. Studies of Field Ionization Using PECVD-grown CNT Tips19. Growth of Carbon Nanotubes for Use in Origami Supercapacitors20. Self-Alignment of Folded, Thin-Membranes via Nanomagnet Attractive Forces21. Control System Design for the Nanostructured Origami™ 3D Nanofabrication Process22. Measuring Thermal and Thermoelectric Properties of Single Nanowires and Carbon Nanotubes23. Nanocomposites as Thermoelectric Materials24. CNT Assembly by Nanopelleting25. Templated Assembly by Selective Removal26. Building Three-dimensional Nanostructures via Membrane FoldingPower MEMS1. Hand-assembly of an Electrospray Thruster Electrode Using Microfabricated Clips2. A Fully Microfabricated Planar Array of Electrospray Ridge Emitters for Space PropulsionApplications3. Thermal Management in Devices for Portable Hydrogen Generation4. Autothermal Catalytic Micromembrane Devices for Portable High-Purity Hydrogen Generation5. Self-powered Wireless Monitoring System Using MEMS Piezoelectric Micro Power Generator6. An Integrated Multiwatt Permanent Magnet Turbine Generator7. Micro-scale Singlet Oxygen Generator for MEMS-based COIL Lasers8. A Thermophotovoltaic (TPV) MEMS Power Generator9. MEMS Vibration Harvesting for Wireless Sensors10. Fabrication and Structural Design of Ultra-thin MEMS Solid Oxide Fuel Cells11. Tomographic Interferometry for Detection of Nafion® Membrane Degradation in PEM Fuel Cells∙The Center for Integrated Photonic Systems (CIPS) mission is to create a meaningful vision of the future, a framework for understanding how technology, industry and business interact and evolve together in the future is required. Models provide us with a process for analyzing the many complex factors that shape this industry and the progress of related technologies.The materials processing center .Making matter meet human needsResearchThe Center brings together MIT faculty and research staff from diverse specialties to collaborate on interdisciplinary materials problems. Center research involves over 150 faculty, research staff, visiting scientists, and graduate and undergraduate students.MPC researchers cover the full range of advanced materials, processes, and technologies, including∙electronic materials∙batteries & fuel cells∙polymers∙advanced ceramics∙materials joining∙composites of all types∙photonics∙electrochemical processing ∙traditional metallurgy∙environmental degradation∙materials modeling- many scale ∙materials systems analysis∙nanostructured materials∙magnetic materials and processes ∙biomaterials∙materials economicsFaculty ProfilesA.I. AkinwandeFlat panel displays,Vacuum Microelectronics and its application to flat panel displays, RF power sources, and sensors. Wide bandgap semiconductors and applications to flat panel displays, UV emitters and RF power sourcesView current research abstracts (pdf)G. BarbastathisBiomedical design instrumentation; precision engineering robotics; volume holographic architectures for data storage, color-selective tomographic imaging, and super-resolving confocal microscopy; interferometric surface characterization; and adaptive micro-opto-mechanics. Optical MEMS.View current research abstracts (pdf)View group web siteM. BazantResearch focuses on transport phenomena in materials and engineering systems, especially diffusion coupled to fluid flow. My group is currently studying granular flow in pebble-bed nuclear reactors, nonlinear electrokinetic flows in microfludic devices, ion transport in thin-film lithium batteries, and advection-diffusion-limited aggregation.View current research abstracts (pdf)View group web siteS. BhatiaResearch focuses on applications of micro- and nanotechnology to tissue repair and regeneration. Emphasis on development of microfabrication tools to improve cellular therapies for liver disease, living cell arrays to study stem cell biology, and nanoparticles for cancer diagnosis and treatment.View current research abstracts (pdf)View group web siteD. BoningSemiconductor manufacturing. Modeling and control of chemical mechanical polishing. Variation modeling and reduction in fabrication processes, devices, and interconnects. Run by run and feedback control for quality and environment in semiconductor fabrication. Software systems for distributed and collaborative computer aided design and fabrication.View current research abstracts (pdf)View group web siteA.P. ChandrakasanDesign of digital integrated circuits and systems. Emphasis on the energy efficient implementation of distributed microsensor and signal processing systems. Protocols and Algorithms for Wireless Systems. Circuits techniques for deep sub-micron technologies.View current research abstracts (pdf)View group web siteG. ChenMicro- and nanoscale heat transfer and energy conversion with applications in thermoelectrics, photonics, and microelectronics; nano-mechanical devices and micro-electro-mechanical systems; radiation and electromagnetic metamaterials.View current research abstracts (pdf)View group web siteM. CulpepperResearch focuses on precision interfaces, precision manufacturing, design for manufacturing, applying precision principles as enabling technologies in multi-disciplinary product design: electronic test equipment, automotive systems, precision compliant mechanisms.View current research abstracts (pdf)View group web siteL. DanielResearch focuses on engineering design applications to drive research in simulation and optimization algorithms and software, design of microfabricated inductors.View current research abstracts (pdf)View group web siteP. DoyleUnderstanding the dynamics of single polymers and biomolecules under forces and fields; lab-on-chip separations, polymer rheology. DNA electrophoresis in microdevices. Superparamagnetic colloids. Brownian Dynamics simulations of complex molecules. Microheology of biopolymers.View current research abstracts (pdf)View group web siteA. EpsteinSmart engines, turbine heat transfer and aerodynamics, advanced diagnostic instrumentation, turbomachinery noise, environmental impact of aircraft.View current research abstracts (pdf)View group web siteD. FreemanBiological micromechanics, MEMS, light microscopy and computer microvision.View current research abstracts (pdf)牋牋牋牋牋牋牋牋牋牋牋?牋View group web siteM. GrayMicrofabricated devices for use in diagnostic medicine and biological research. Particle and fuid analysis of flowing media using absorbance and fluorescence techniques as a means for understanding cell or organism metabolism and phenotypic expression.View group web siteJ. HanBioMEMS, biomolecule analysis, micro/nanofluidics, micro-analysis systems.View current research abstracts (pdf)View group web siteJ. JacobsonDevelopment of processes for directly and continuously printing communication, computation, and displays onto arbitrary substrates. Electronic control of biomolecules.View group web siteK. JensenMicrofabrication and characterization of devices and systems for chemical synthesis and detection, hydrocarbon fuel conversion to electrical energy, bioprocessing and bioanalytics. Multiscale simulation of transport and reaction processes. Chemical vapor deposition of polymer, metal, and semiconductor thin films. Synthesis and characterization of quantum dot composite materials.View current research abstracts (pdf)View group web siteR. KarnikMicro- and nanofluidic systems. Application of transport phenomena in nanofluidics for flow control, separation, sensing. Microfluidic devices for studying chemical kinetics and nanoparticle synthesis.View group web siteS.G. KimSystems Design and Manufacturing, MEMS for optical beam steering, microphotonic packaging and active alignment, micro power generation, massive parallel positional assembly of nanostructures, and nano actuator array.View current research abstracts (pdf)View group web siteJ.H. LangAnalysis, design and control of electromechanical systems. Application to traditional electromagnetic actuators, micron scale actuators and sensors, and flexible structures.View current research abstracts (pdf)View group web siteC. LivermoreMicroElectroMechanical Systems (MEMS). Design and fabrication of high power microsystems. Nanoscale self-assembly and manufacturing.View current research abstracts (pdf)View group web siteS. ManalisApplication of micro- and nanofabrication technologies towards the development of novel methods for probing biological systems. Current projects focus on electrical and mechanical detection schemes for analyzing DNA, proteins, and cells.View current research abstracts (pdf)View group web siteD.J. PerreaultAnalysis, design, and control of cellular power converter architectures. DC/DC Converters fordual-voltage electrical systems. Electrical system transient investigation. Exploration of non-conventional electricity sources for motor vehicles.View group web siteM.A. SchmidtMicroElectroMechanical Systems (MEMS). Microfabrication technologies for integrated circuits, sensors, and actuators. Design of microsensor and microactuator systems.View current research abstracts (pdf)A. SlocumPrecision Engineering; Machine Design; Product Design.View current research abstracts (pdf)View group web siteC.V. ThompsonProcessing, structure, properties, performance, and reliability of thin films and structures for micro- and nano-devices and systems. Reliability and Interconnect.View current research abstracts (pdf)View group web siteT. ThorsenIntegrating microfluidic design and fabrication techniques, electronics and optics with biochemical applications. Optimizing channel dimensions, geometry, and layout to generate 3-D fluidic networks that are functional and scalable. Interface development to combine microfluidic technologies with pneumatic valves, MEMS-based detector systems, and software-based data acquisition and interpretation, creating devices for fundamental research and diagnostic applications.View current research abstracts (pdf)View group web siteH.L. TullerCharacterize and understand key electronic, microstructural, and optical properties of advanced ceramic materials. Fabrication andcharacterization of crystals, ceramics and glasses for electronic devices, lasers, electrochemical energy conversion, sensors and actuators.View current research abstracts (pdf)View group web siteJ. VoldmanBiological applications of microsystem technology. Engineering and use of microsystems for analysis and engineering of single cells. Physical and electrical cell manipulation. Design, modeling, microfabrication, and testing of microfluidic biological devices employing unconventional materials and fabrication processes. Electromechanics at the microscale.View current research abstracts (pdf)View group web siteE. N. WangDevelopment of MEMS/NEMS for: Biochemical sensing and detection; Thermal management of high power density and high performance systems; Diagnostics for biological systems and bio-functionality View group web siteB. WardlePower MEMS microyhydraulics, structural health monitoring, nanocomposites, damageresistance/tolerance of advanced composite materials, cost modeling in the structural design process, conversion of technology to value.View current research abstracts (pdf)View group web siteJ. WhiteTheoretical and practical aspects of numberical algorithms for problems in circuit, device, interconnect, packaging, and micromechanical system design; parallel numerical algorithms; interaction between numerical algorithms and computer architecture.View current research abstracts (pdf)View group web siteLaser-cooling brings large object near absolute zeroAnne Trafton, News OfficeApril 5, 2007Using a laser-cooling technique that could one day allow scientists to observe quantum behavior in large objects, MIT researchers have cooled a coin-sized object to within one degree of absolute zero.Fig.1Assistant professor Nergis Mavalvala, left, and Ph.D. student Thomas Corbitt are part of an international team that has devised a way to cool large objects to near absolute zero. Enlarge image (no JavaScript)Fig.Super-mirrorMIT researchers have developed a technique to cool this dime-sized mirror (small circle suspended in the center of large metal ring) to within one degree of absolute zero. Enlarge image (no JavaScript)Fig.2Assistant professor Nergis Mavalvala, right, and Ph.D. student Thomas Corbitt look over the laser system they use to cool a coin-sized mirror to within one degree of absolute zero. Enlarge image (no JavaScript)。
基于模型分块逼近的三关节机器人鲁棒滑模控制马莉丽;钟斌【摘要】三关节机器人结构参数、作业环境的外界干扰及结构振动等不确定因素均会造成其动力学模型不确定,导致机器人关节位置镇定或轨迹跟踪控制器的设计具有一定的难度。
为此,设计三个RBF(Radical Basis Function)神经网络分别对机器人不确定模型中的三个不确定项进行分块逼近,得到三个不确定项的估计信息,从而得出机器人估计模型,神经网络的权值采用适应算法。
针对机器人估计模型设计鲁棒滑模控制律,其中鲁棒项用于克服神经网络建模误差。
通过定义 Lya-punov函数,证明了控制系统是稳定的。
实验结果也表明了三关节均约在1 s时达到期望位置或跟踪期望轨迹,位置镇定误差或轨迹跟踪误差也快速、稳定地趋于零。
%Generally,the dynamic model of robot with three-j oint is undetermined due to three-j oint robot’s uncertain structure parameters,working environment’s external interfere and struc-tural vibration.Accordingly,it is difficult to control the robot’s joints’position stabilizing and traj ectory tracking and controller’s design due to the dynamic model’s uncertainty.Therefore, three designed RBF(Radical Basis Function)neural networks are used to respectively model the three undetermined terms of the undetermined robot dynamic model,with partition approxima-ting the three-joint robot.Three undetermined terms’estimation information is respectively ob-tained,with the robot’s estimation model obtained.The neural networks’weights are obtained through the adaptive algorithm.The robust sliding mode control law is designed based on the ro-bot’s estimation model.The control law’srobust term is used to overcome the neural networks’ modeling er ror.The control system’s stability is proved by defining Lyapunov function.The simulation experiments test verifies that three joints can trace ideal trajectory and reach an ideal position in 1 s,and stabilization error and tracking error can fast and stably approximate to zero.【期刊名称】《西安理工大学学报》【年(卷),期】2016(032)004【总页数】6页(P437-442)【关键词】三关节机器人;模型分块逼近;关节控制;RBF神经网络【作者】马莉丽;钟斌【作者单位】中国人民武装警察部队工程大学装备工程学院,陕西西安 710086;中国人民武装警察部队工程大学装备工程学院,陕西西安 710086【正文语种】中文【中图分类】TP242.2三关节机器人(以下简称机器人)结构紧凑,所占空间小,灵活性强,工作空间较大,避障性好,广泛应用于工业机器人中。
No.4Apr.2021第4期2021年4月组合机床与自动化加工技术Modular Machine Tool & Automatic Manufacturing Techninue文章编号:1001 -2265(2021)04 -0096 -04DOI : 10.13462/j. cnki. mmtamt. 2021.04. 023伺服系统转动惯量辨识及控制器PI 参数优化孙彦瑞,苏成志(长春理工大学机电工程学院,长春130000)摘要:在机器人运行时,为了使伺服电机在最优性能下达到目标速度、在工作过程中有着更强的抗 扰动能力,并避免出现震荡、谐振的状况,从而造成机器人运行时动态稳定性严重降低。
提出一种 基于非线性动态学习因子的粒子群优化算法,对普通粒子群优化算法进行改进。
该算法以伺服系 统控制模型中的速度控制器为核心,实时辨识负载转动惯量值,使伺服系统内部控制参数根据实际 工况调节;运用该辨识值,通过计算得到速度控制PI 参数值,并实时修正速度控制器PI 参数值。
MATLAB/SIMULINK 仿真结果表明,与传统的粒子群优化算法相比,无论在电机启动过程中、还是 负载扰动下,该方法都具有更快的响应速度、更高的控制精度以及更强的抗干扰能力。
关键词:转动惯量;非线性动态学习因子;粒子群优化算法;速度控制器PI 参数中图分类号:TH166 ;TG506 文献标识码:AServo System Inertia IdenhPcahon and Controller PI Parameter OptimizationSUN Yan-rui , SU Cheng-zhi(School of Mechanical and Electrical Engineering , Changchun Univvrsity of Science and Technolo/y , Changchun 130000, Ch/ia )Abstrach : During the operation of the robot , in order to make the servo motor achieve the target speed un der the optimal performance , and have stronger anti-disirbance ability in the working proces s , and to a void the prob —m of vibration and resonance , resulting in a serous reduction in the dynamic stability of the robot. The coniol model of servo motor is analyzed , and a particle swarm optimization algorithm based on nonlmear dynamic learning factor is proposed. The algorithm ties the speed conioller in the servo system coniol model as the core , and can identify the loadz moment of inertia in real time , so that the internaicontrol parameters of the s ervo system can be adjusted according to the acial condbions. By using the i dentification value , the PI parameter value of the speed control is obtained through calculation , and the PI parameter value of the speed conioller is corrected in real time. The results of MATLAB/SIMULINK sim ulation show that compared with the traditional pakWle swarm optimization algorithm , this method has fas ter response speed , higher control accuracy and stronger anti-interference ability , whether in the motorsha+hing p+oce s o+unde+hheload dishu+bance.Key wois : moment of inertia ; nonlinear dynamic learning factor ; particle swarm optimization tgoriim ; speed conho l e+PIpa+amehe+0引言机器人在运行时,每个轴的负载转动惯量与负载 扭矩随着机器人的姿态的变化而变化;伺服系统对负 载转动惯量的辨识精度、辨识快慢,决定着伺服系统运 行的稳定性、精确性与快速性。
六旋翼飞行器建模及位置跟踪控制王伟;邱启明【摘要】为实现六旋翼的位置跟踪与控制功能,对六旋翼飞行器的数学模型进行了分析,通过线性化得到了其简单数学模型。
在简化的数学模型基础之上设计了基于PID(比例-积分-微分控制器)控制算法的姿态控制器和位置控制器,控制器仿真结果表明位置跟踪误差小于2%。
飞行实验中飞行器准确追踪给定的姿态角精度大于80%,飞行器性能稳定,实现方法合理。
%In order to accomplish control functions,a simple mathematical model was achieved after the model of six-rotor unmanned aerial( UAVs) vehicle was analyzed and linearnized. Attitude controller and position controller was designed based on PID ( Proportional-Integral-Derivative ) control algorithm and the simply mathematical mentioned above. The results of simulation putted on position controller showed that position error is less than two percent. The degree of accuracy on the fact that the reference input was correctly traced by UAVs is greater than eighty percent during the flight test. The performance is stable,and the implementation method is reasonable.【期刊名称】《电子器件》【年(卷),期】2014(000)003【总页数】7页(P507-513)【关键词】控制工程;位置跟踪;PID控制;数学建模;姿态控制【作者】王伟;邱启明【作者单位】南京信息工程大学信息与控制学院,南京210044;南京信息工程大学信息与控制学院,南京210044【正文语种】中文【中图分类】V249近些年来,无人机(Unmanned Aerial Vehicle)在救援、安保、巡查和航拍等方面的广泛应用已引起人们的广泛关注,这些应用对无人机的稳定悬浮、操作灵活和安全等性能提出了极大挑战。
第42卷第6期2021年6月Vol.42,No.6Jun.2021东北大学学报(自然科学版)Journal of Northeastern University(Natural Science)doi:10.12068/j.issn.1005-3026.2021.06.022广义非线性脉冲切换系统的指数稳定和l2增益控制杨冬梅,李祉含(东北大学理学院,辽宁沈阳110819)摘要:研究了一类具有脉冲的广义非线性切换系统的指数稳定问题和厶增益控制问题.将脉冲以及非线性控制加入到系统当中,系统更具有实际意义.首先,提岀了一种具有厶增益控制的状态反馈控制器的有效设计方法,通过构建Lyapunov函数,改进系统中的状态反馈控制器,使得闭环系统是指数稳定的.其次,利用线性矩阵不等式并结合模型依赖平均驻留时间方法,给岀了系统指数稳定且具有厶增益性能的充分条件.最后,通过数值例子及图像仿真来说明理论结果的有效性.关键词:广义系统;指数稳定性;Lyapunov函数;厶增益;脉冲;平均驻留时间中图分类号:O231文献标志码:A文章编号:1005-3026(2021)06-0908-05Exponential Stability and L2-Gain Control of Nonlinear Pulse Switching Singular SystemsYANG Dong-mei,LI Zhi-han(School of Sciences,Northeastern University,Shenyang110819,China.Corresponding author:LI Zhi-han, E-mail:1208335717@)Abstract:Exponential stability and L2-gain control of singular nonlinear switching systems with pulses are studied.The pulse and nonlinear control are added to the system to make it of more practical significance.First,an effective design method of state feedback controller with L2-gain control is proposed by constructing the Lyapunov function,and the state feedback controller in the system is improved to make the closed-loop system exponentially stable.Secondly,by using the linear matrix inequality and the model dependent average dwell time method,the sufficient conditions for exponential stability and L-gain performance are given.Finally,numerical examples and image simulation are given to illustrate the effectiveness of the theoretical results. Key words:singular system;exponential stability;Lyapunov function;L-gain;pulse;average dwell time切换系统与广义系统的结合[|]作为一类混杂系统的重要模型广泛存在于许多工程领域中,比如:经济系统、电力系统、高速交通系统、容错控制系统[2]、飞行器控制系统等.从理论分析和工程实践的角度,切换广义系统受到众多学者的青睐.另一方面,虽然已经有很多方法用于广义系统的求解,但是求解以外,更多人关注广义系统控制的相关问题,因此研究广义系统控制的求解等相关问题是十分必要的.实际系统在连续性和离散性中有着错综复杂的交集,在实际动态过程中,系统在某一时刻的突然变化往往会导致脉冲行为,因此通过建立切换广义脉冲非线性系统的复杂模型,对其控制性能以及稳定性能进行研究.文献[3]设计了切换线性系统的动态输出反馈,文献[4-5]分别讨论了切换广义系统的脉冲和时滞问题.由于实际系统更复杂,存在更多的不确定性,所以本文首先将系统复杂化,设计了相比于传统的输出反馈控制更收稿日期:2020-09-24基金项目:国家自然科学基金资助项目(61673100).作者简介:杨冬梅(1966-),女,辽宁沈阳人,东北大学教授.第6期杨冬梅等:广义非线性脉冲切换系统的指数稳定和厶2增益控制909有效的状态反馈控制器,通过状态反馈控制器得到的输出信号都是可靠的,不存在延迟,并且能够在不改变系统能控性的同时使得系统稳定正常工作,获得期望的性能.最后利用线性矩阵不等式的算法来解决针对广义系统中含有等式约束求解的难题,使结论更具有一般性.稳定性一直是研究的焦点问题,其中指数稳定比渐进稳定更加适用于广义系统,文献[6-7]分别研究了离散马尔可夫跳跃广义系统的鲁棒稳定和不确定广义非线性系统的指数稳定,通过对比其他文献结论得出指数稳定更有助于分析系统解的收敛速率.本文主要研究具有脉冲的一类广义非线性切换系统的稳定性问题和厶2增益控制•给出了状态反馈控制器设计的有效方法,提出了确保系统指数稳定性和加权厶2增益的充分条件•算例仿真中,可通过求解矩阵不等式得到控制器增益矩阵及控制参数,证明理论结果的可行性.1问题描述考虑一系列具有脉冲的广义非线性切换系统:应⑴=£(”x(r)+B”®“⑺+码(必(”(r,x(r))+'―)t),t^t k.>△x=X(t k)—X(t k)=①*X(t),t=t”.z(t)=。
第2期 收稿日期:2020-09-18作者简介:韩雨雪(1995—),河北张家口人,硕士研究生,研究方向,生物质脱碳及沼气提纯等。
中国沼气提纯技术发展现状韩雨雪1,陈彬剑1,赵 晶2(1.山东建筑大学,山东济南 250000,2.济宁生态环境监控中心,山东济宁 273100)摘要:沼气作为一种新兴的清洁可再生能源,其提纯生产的生物天然气可以代替传统天然气,从而根本上解决天然气供需紧张的问题。
同时发展生物天然气是农业生产废弃物的资源化利用,也是响应国家推动清洁能源发展的号召。
CO2作为一种惰性气体是影响沼气使用效果的最主要因素,CO2不具有可燃性,而且体积分数较大,降低了沼气的热值。
因此制备生物天然气的核心去除沼气中的CO2,提高燃烧性能。
本文论述了近年来常见的天然气脱碳提纯技术,介绍了各种方法的脱碳提纯原理、应用及限制条件。
重点阐明了真空变压吸附法(VPSA)在天然气脱碳中的地位及工业应用,指出了VPSA未来研究方向,为今后生物天然气的工业广泛应用提供了理论依据。
关键词:生物天然气;沼气提纯;发展前景中图分类号:S216.4 文献标识码:A 文章编号:1008-021X(2020)02-0067-02 随着我国现代化进程的推进,能源需求不断增加,能源消费仍以传统煤燃料为主。
但是大量的煤炭的使用会造成粉尘污染,破坏生态。
因此国家发改委在《能源发展“十三五”规划》中明确提出,“十三五”期间增加对天然气的使用,到2020年天然气消费比重力争达到10%。
但是我国天然气市场储存已无法满足其需求,造成天然气的对外依存度不断提高。
因此,可替代天然气的可再生能源的研究与开发受到了越来越多的关注。
尤其是将废弃生物质高效转化为生物天然气,具有保护环境和节能减排的多重意义。
沼气作为优质清洁能源,是对生物质能的高效益利用。
中国的沼气最早应用于20世纪20年代,用于农村家庭的炊事,经过近百年的发展,由幼稚走向成熟,当下正面临高速发展时期。
基于MATLAB的智能PID控制器设计与仿真摘要在工业生产中应用非常广泛的是PID控制器,是最早在经典控制理论基础上发展起来的控制方法,应用也十分广泛。
传统的PID控制器原理十分简单,即按比例、积分、微分分别控制的控制器,但是他的核心也是他的难点就是三个参数(比例系数Kp、积分系数Ki、微分系数Kd)的整定。
参数整定的合适,那么该控制器将凭借结构简单、鲁棒性好的优点出色的完成控制任务,反之则达不到人们所期望的控制效果。
人工神经网络模拟人脑的结构和功能而形成的信息处理系统,是一门十分前沿高度综合的交叉学科,并广泛应用于工程领域。
神经网络控制是把自动控制理论同他模仿人脑工作机制的数学模型结合起来,并拥有自学习能力,能够从输入—输出数据中总结规律,智能的处理数据。
该技术目前被广泛应用于处理时变、非线性复杂的系统,并卓有成效。
关键词自适应PID控制算法,PID控制器,神经网络Design and simulation of Intelligent PID Controllerbased on MATLABAbstractPID controller ,the control method which is developed on the basis of classical control theory, is widely used in industrial production.The Principle of traditional PID controller is very simple, which contains of the proportion, integral, differential three component, but its core task and difficulties is three parameter tuning(proportional coefficient Kp, integral coefficient Ki and differential coefficient KD).If the parameter setting is suitable, the controller can accomplish the control task with the advantages of simple structure and good robustness;but on the contrary, it can not reach the desired control effect which we what.Artificial neural network , the formation of the information processing system which simulate the structure and function of the human brain , is a very high degree of integration of the intersection of disciplines, and widely used in the field of engineering. Neural network control ,combining automatic control theory and the imitate mathematical model of the working mechanism of human brain , has self-learning ability, and can summarize the law of the input-output data , dealing with data intelligently .This technique has been widely used in the process of time-varying, nonlinear and complex system, and it is very effective.Key W ord:Adaptive PID control algorithm,PID controller,Neural network目录摘要 (I)Abstract (II)第一章绪论 (1)1.1 课题研究背景及意义 (1)第二章 PID控制器 (2)2.1 PID控制原理 (2)2.2常规PID控制器的算法理论 (3)2.2.1 模拟PI D控制器 (3)2.2.2 数字P I D控制算法 (3)2.2.3常规PID控制的局限 (5)2.2.4 改进型PID控制器 (5)第三章人工神经网络 (8)3.1 人工神经网络的原理 (8)3.2神经网络PID控制器 (8)3.2.1神经元PID控制器 (8)3.2.2 单神经元自适PID应控制器 (9)3.3 BP神经网络参数自学习的PID控制器 (12)第四章MATAB仿真 (16)4.1 仿真过程 (16)第五章结论与展望 (24)致谢 (25)参考文献 (25)华东交通大学毕业设计(论文)第一章绪论1.1 课题研究背景及意义在工业生产中应用非常广泛的是PID控制器,是最早在经典控制理论基础上发展起来的控制方法,应用也十分广泛。
A New Solution For Coupled Simulation Of Multi-Body Systems And Nonlinear Finite Element Models Giancarlo CONTI, Tanguy MERTENS, Tariq SINOKROT(LMS, A Siemens Business)Hiromichi AKAMATSU, Hitoshi KYOGOKU, Koji HATTORI(NISSAN Motor Co., Ltd.)1 IntroductionOne of the most common challenges for flexible multi-body systems is the ability to properly take into account the nonlinear effects that are present in many applications. One particular case where these effects play an important role is the dynamic modeling of twist beam axles in car suspensions: these components, connecting left and right trailing arms and designed in a way that allows for large torsional deformations, cannot be modeled as rigid bodies and represent a critical factor for the correct prediction of the full-vehicle dynamic behavior.The most common methods to represent the flexibility of any part in a multi-body mechanism are based on modal reduction techniques, usually referred to as Component Mode Synthesis (CMS) methods, which predict the deformation of a body starting from a preliminary modal analysis of the corresponding FE mesh. Several different methods have been developed and verified, but most of them can be considered as variations of the same approach based on a limited set of modes of the structure, calculated with the correct boundary conditions at each interface node with the rest of the mechanism, allowing to greatly reduce the size of system’s degrees of freedom from a large number of nodes to a small set of modal participation factors. By properly selecting the number and frequency range of the modes, as well as the boundary conditions at each interface node [1], it is possible to accurately predict the static and dynamic deformation of the flexible body with remarkable improvements in terms of CPU time: this makes these methods the standard approach to reproduce the flexibility of components in a multi-body environment. Still, an important limitation inherently lies in their own foundation: since displacements based on modal representation are by definition linear, any nonlinear phenomena cannot be correctly simulated. For example, large deformations like twist beam torsion during high lateral acceleration cornering maneuvers typically lead to geometric nonlinearities, preventing any linear solution from accurately predicting most of the suspension’s elasto-kinematic characteristics like toe angle variation, wheel center position, vertical stiffness.One possible solution to overcome these limitations while still working with linear modal reduction methods is the sub-structuring technique [2]: the whole flexible body is divided into sub-structures, which are connected by compatibility constraints preventing the relative motion of the nodes that lie between two adjacent sub-structures. Standard component mode synthesis methods are used in formulating the equations of motion, which are written in terms of generalized coordinates and modal participation factors of each sub-structure. The idea behind it is that each sub-portion of the whole flexible structure will undergo smaller deformations, hence remaining in the linear flexibility range. By properly selecting the cutting sections it is usually possible to improve the accuracy of results (at least in terms of nodal displacements: less accuracy can be expected for stress and strain distribution). Another limitation of these methods is the preliminary work needed to re-arrange the FE mesh, although some CAE products already offer automatic processes enabling the user to skip most of the re-meshing tasks and hence reducing the modeling efforts.An alternative approach to simulate the behavior of nonlinear flexible bodies is based on a co-simulation technique that uses a Multi-body System (MBS) solver and an external nonlinear Finite Element Analysis (FEA) solver. Using this technique one can model the flexible body in the external nonlinear FEA code and the rest of the car suspension system in the MBS environment. The loads due to the deformation of the body are calculated externally by the FEA solver and communicated to the MBS solver at designated points where the flexible body connects to the rest of the multi-body system. The MBS solver, on the other hand, calculates displacements and velocities of these points and communicates them to the nonlinear FEA solver to advance the simulation. This approach doesn’t suffer from the limitations that arise from the linear modeling of the flexibility of a body. This leads to more accurate results, albeit at the price of much larger CPU time. In fact, simulation results are strongly affected by the size of the communication time step between the two solvers: a better accuracy (and more stable solver convergence) can be generally obtained by using smaller time steps which require larger calculation times, as shown also in [3].2 Overview of the activityThis paper presents the results of a benchmark activity performed in collaboration with Nissan Auto where a new FE-MBS variable-step co-simulation technique was used: a coupling at the iteration level currently implemented in commercial FEA package LMS SAMCEF Mecano [4] and general purpose multi-body system package LMS b Motion [5]. In this technique each solver uses its own integrator but only one Newton solver is used. In this case one solver is designated as the master and will be responsible for solving the Newton iterations. The coupled iterations continue until both solvers satisfy their own solution tolerances and convergence is achieved. The co-simulation process is organized by means of a supervisor code that manages the data exchange and determines the new time step of integration for both solvers. Further technical details on this “coupled simulation“ method, as well as a comparison with the variable-step co-simulation method, are available in [6].A multi-body model of a rear twist beam suspension has been created, where the flexibility of the twist beam was simulated with three alternative modeling techniques to be compared:- Component Mode Synthesis (Craig-Bampton method)- Linear sub-structuring- Nonlinear FE-MBS coupled simulation.As a further step also the two bushings connecting the twist beam with the car body, originally modeled in b Motion as standard force elements with nonlinear stiffness and damping characteristics for all directions, have been replaced by two SAMCEF Mecano nonlinear flexible bodies.Two different suspension events have been simulated in order to compare the results from the different modeling methods:- Suspension roll (opposite wheel vertical travel applied at wheel centers)- Braking in turn (dynamic loads applied at wheel centers).Figure 1 shows the b Motion suspension model used for this activity, where the FE mesh models of twist beam and bushings are also displayed:3 Modeling and simulations3.1 Model validationAs a first step a multi-body model of rear suspension was created in b Motion with input data provided by Nissan Auto from a pre-existing model developed with another multi-body software package: hardpoints location, bodies mass and inertia data, kinematic and compliant connections characteristics, properties of coil springs, shock absorbers, end stop elements. Since the original model included a flexible twist beam based on a modal reduction method (Craig-Bampton) the same original mode set has been used to obtain a linear flexible representation of the twist beam in b Motion. Then a suspension roll has been simulated in both environments in order to validate Motion results with the data from the source model, obtained by applying a vertical displacement in opposite directions at the two wheel centers. The main elasto-kinematic suspension characteristics have been compared: toe and camber variation, wheel center longitudinal and lateral displacements, vertical stiffness. In fig.2 the vertical force at wheel center and the toe angle variation are plotted versus the wheel vertical displacement: the differences between the two models are negligible.Fig. 1b Motion multi-body model of rear suspension with flexible twist beam and bushings3.2 Flexible twist beam modeling Once validated the b Motion model, the linear flexible twist beam was replaced by the two alternative modeling methods intended to take into account the geometric nonlinearities due to the large deformations of the beam element: sub-structuring and coupled simulation Motion – Mecano.- Sub-structuring: the twist beam was cut in3 sections along the central pipe, resultingin 4 separate linear flexible bodies: the twolongitudinal arms + two symmetric halves ofthe beam. Figure 3 shows the three cuttingsections used.- Coupled simulation Motion – Mecano -starting from the original Nastran FE mesh, the dynamic behavior of the full twist beam is calculated by the SAMCEF Mecano nonlinear solver through a specific Analysis Case added to the VL Motion model.3.3 FE bushings modelingAs a further task of the activity, starting from the CAD representation of the geometry of the bushings connecting the twist beam with the car body a Mecano FE model of each bushing has been created and implemented into the b Motion mechanism to replace the original bushing force elements, modeled as nonlinear stiffness and damping curves in all six directions. Material properties for the rubber and metal parts of the bushings were not known in detail, so tentative values have been used for the rubber whereas the metal parts have been considered as rigid: although these assumptions were expected to have a major impact on results, the main purpose of this task was not to obtain accurate and correlated results, rather to prove the capability of the Motion-Mecano coupled simulation method to successfully solve multiple nonlinear flexible bodies in the same model.3.4 Results comparisonFigure 4 shows the results of the suspension roll analysis for two of the most relevant outputs for the handling performance of a car: toe angle and wheel track variation, plotted vs. left wheel vertical displacement. The main outcome is that sub-structuring and coupled Motion-Mecano simulation (not including FE bushings) give very similar results, both different from the linear case: as expected, the linear approach gives reliable results only in a limited range of displacements, whereas for larger deformations of the twist beam a more accurate prediction of the behavior of the system can be obtained only by considering the nonlinear flexibility of the body.In Fig.5 some of the results from the dynamic braking-in-turn maneuver are displayed, where during a cornering maneuver started at around 0.7s a braking force is applied after 1.5s. In this comparison the additional case with the two nonlinear FE bushings is also displayed: again, a remarkable difference can be detected between the linear case and the nonlinear FE-MBS coupled simulation; furthermore a clear effect from nonlinear FE bushings can be seen, although most likely affected by uncertainties on the material properties applied in the Mecano FE bushing models.Fig. 3 Sub-structuring of the linear flexible twist beam Fig. 2Comparison of results between b Motion model and source MBS model4 ConclusionsIn this paper the usage of a new FE-MBS co-simulation technique for an automotive application is compared with two alternative solutions to represent the nonlinear flexibility of a body in a multi-body mechanism. A b Motion rear suspension model with flexible twist beam has been created with the aim to simulate two typical handling events where the proper prediction of the large deformation of the twist beam strongly affects most of the elasto-kinematic characteristics of the suspension. The compared results show a clear difference between the linear approach, based on a modal representation of the flexibility of the body, and the alternative methods which allow a more correct prediction of the geometric nonlinearity.This new b Motion – SAMCEF Mecano co-simulation technique allows also the simulation of multiple nonlinear flexible bodies in the same mechanisms as shown in this paper. Further studies are currently on-going to extend the usage of this solution to complex applications like flexible contact and friction forces, nonlinear material properties, thermal effects.5 References[1] Yoo W.S., Haug E.J.: “Dynamics of flexible mechanical systems using vibration and static correctionmodes ”, Journal of Mechanisms, Transmissions and Automation in Design, 108, 315-322, 1985[2] Sinokrot T.Z., Nembrini M., Toso A., Prescott W.C.: "A Comparison Of Sub-Structuring Synthesis And TheCosimulation Approach In The Dynamic Simulation Of Flexible Multi-body Systems ", MULTIBODYDYNAMICS 2011, ECCOMAS Thematic Conference, Brussels, Belgium, 4-7 July 2011[3] Sinokrot T.Z., Nembrini M., Toso A., Prescott W.C.: "A Comparison Of Different Multi-body SystemApproaches In The Modeling Of Flexible Twist Beam Axles ", Proceedings of the 8th International Conference on Multi-body Systems, Nonlinear Dynamics, and Control, August 28-31, 2011, Washington D.C., USA[4] LMS International, b Online Help Manual , 2013.[5] LMS Samtech, Samcef Online Help Manual – version 15.1, 2013.[6] Sinokrot T., Jetteur P., Erdelyi H., Cugnon F., Prescott W.: "A New Technique for Stronger Couplingbetween Multi-body System and Nonlinear Finite Element Solvers in Co-simulation Environments ",MULTIBODY DYNAMICS 2013, ECCOMAS Thematic Conference, Zagreb, Croatia, 1-4 July 2013Fig. 4Suspension roll analysis: toe angle and wheel track variationsFig. 5Braking-in-turn analysis: wheel base and toe angle variations。
扬州市人民政府关于2017-2019年度扬州市自然科学优秀学术论文评选结果的通报
文章属性
•【制定机关】扬州市人民政府
•【公布日期】2021.03.05
•【字号】扬府发〔2021〕16号
•【施行日期】2021.03.05
•【效力等级】地方规范性文件
•【时效性】现行有效
•【主题分类】科技成果与知识产权
正文
市政府关于2017-2019年度扬州市自然科学优秀学术论文评选结果的通报-市政府文件-政府办
各县(市、区)人民政府,经济技术开发区、生态科技新城、蜀冈—瘦西湖风景名胜区管委会,市各委办局(公司),市各直属单位:
为提高我市自然科学学术水平,鼓励全市科技工作者开展学术创新服务发展,促进全市科技人才成长,2020年我市开展了2017-2019年度扬州市自然科学优秀学术论文评选工作,共征集到701篇论文,其中675篇论文通过资格审查。
经评审委员会评定,分理工类、农业类、医药类、管理教育类,共评出优秀学术论文269篇,其中一等等次33篇、二等等次101篇、三等等次135篇。
经研究,市政府决定对评选出的269篇优秀学术论文给予通报并颁发证书。
希望全市各级科技团体和广大科技工作者,以科技赋能产业为己任,积极开展学术研究,主动投身科技创新,脚踏实地,严谨求是,把“好地方”扬州建设得好上加好、越来越好做出积极贡献。
附件:2017-2019年度扬州市自然科学优秀学术论文评选结果
扬州市人民政府
2021年3月5日附件
2017-2019年度扬州市自然科学优秀学术论文评选结果
一等等次(33篇)
二等等次(101篇)
三等等次(135篇)。
第30卷第14期2022年7月Vol.30No.14Jul.2022光学精密工程Optics and Precision Engineering压电定位平台Hammerstein建模与反馈线性化控制黄涛1,罗治洪1,陶桂宝1*,凌明祥2*(1.重庆大学机械与运载工程学院,重庆400044;2.中国工程物理研究院总体工程研究所,四川绵阳621999)摘要:压电定位平台以压电陶瓷、柔性铰链作为驱动及放大机构,具有高定位精度和快响应速度,被广泛应用于各种精密/超精密定位领域。
压电定位平台面临的主要挑战是压电陶瓷的固有迟滞非线性特性,这严重影响平台的定位和跟踪精度。
针对此问题,提出一种基于Hammerstein结构的迟滞建模方法及基于此模型的输入-输出反馈线性化控制策略。
首先,建立Hammerstein结构的迟滞模型,并进行模型参数估计。
接着,以基于Hammerstein模型的输入-输出反馈线性化控制策略设计跟踪控制器。
最后,在压电定位平台上对建立的模型和设计的跟踪控制器进行实验验证。
模型辨识实验结果表明:提出的Hammerstein模型能有效地拟合压电定位平台输入量与输出量之间的迟滞非线性特性,其均方根误差小于0.5μm。
轨迹跟踪实验结果表明:设计的跟踪控制器对期望信号(幅值60μm,频率100Hz)的跟踪均方根误差为0.9266μm,相较于基于改进的速率相关PI(Modified Rate-dependent Prandtl-Ishlinskii,MRPI)模型的前馈补偿跟踪控制、基于MRPI模型的前馈补偿与PID反馈复合跟踪控制,精度分别提高81.22%、46.25%。
关键词:压电陶瓷;压电定位平台;迟滞非线性;Hammerstein模型;反馈线性化控制中图分类号:TP391.4;TH691.9文献标识码:A doi:10.37188/OPE.20223014.1716 Hammerstein modeling and feedback linearization control forpiezoelectric positioning stageHUANG Tao1,LUO Zhihong1,TAO Guibao1*,LING Mingxiang2*(1.College of Mechanical and Vehicle Engineering,Chongqing University,Chongqing400044,China;2.Institute of Systems Engineering,China Academy of Engineering Physics,Mianyang621999,China)*Corresponding author,E-mail:ling_mx@,gbtao@Abstract:A piezoelectric positioning stage is driven and amplified by piezoelectric ceramic and flexible hinges,which can provide high positioning accuracies and response speeds.Thus,it is widely used in vari⁃ous precision/ultra-precision positioning fields.However,the primary challenge presented by the piezo⁃electric positioning stage is the inherent hysteresis nonlinear characteristics of piezoelectric ceramics,which significantly affects the positioning and tracking accuracy of the piezoelectric positioning stage.Hence,a hysteresis modeling method based on the Hammerstein structure and an input-output feedback linearization control strategy is proposed herein.First,hysteresis modeling based on the Hammerstein structure is pro⁃posed,and the parameters are estimated.Subsequently,based on the Hammerstein model,a tracking controller is designed via an input–output feedback linearization control strategy.Finally,the proposed 文章编号1004-924X(2022)14-1716-09收稿日期:2022-04-07;修订日期:2022-05-10.基金项目:国家重点研发计划项目(No.2018YFB1701203);国家自然科学基金项目(No.52075179)第14期黄涛,等:压电定位平台Hammerstein建模与反馈线性化控制Hammerstein model and the designed tracking controller are experimentally verified on a piezoelectric posi⁃tioning stage.The experimental results of model identification reveal that the proposed Hammerstein mod⁃el can effectively fit the hysteresis nonlinearity between the input and output of the piezoelectric positioning stage and that its root mean square error is less than0.5μm.Meanwhile,the experimental results of tra⁃jectory tracking indicate that the designed tracking controller can track the desired signal(amplitude60μm;frequency100Hz)with a root mean square error of0.9266μpared with the feedforward compensation tracking control based on the modified rate-dependent Prandtl-Ishlinskii(MRPI)model and the compound tracking control of feedforward compensation based on the MRPI model and proportional-in⁃tegral-derivative feedback,the proposed model offers an accuracy improvement of81.22%and46.25%,respectively.Key words:piezoelectric ceramic;piezoelectric positioning stage;hysteresis nonlinearity;hammerstein model;feedback linearization control1引言以压电陶瓷作为驱动元件,以柔性铰链作为导向放大机构的压电定位平台能够提供高定位精度和快响应速度,已广泛应用于微机械制造、微型零件的操作与装配、超精密加工、生物工程、生命与医疗科学、光学调整、原子力显微镜、扫描隧道显微镜、半导体制造设备以及光电等领域[1]。
M-9Temperature, Process andStrain MetersDPi32, shown smaller than actual size.DPi16, shownsmaller than actual size.DPi8, shown smaller than actual size.The OMEGA ® iSeries is a family of microprocessor-based instruments offered in three true DIN sizes with NEMA 4 (IP65) rated front bezels. All of the instruments share the same set-up and configuration menu and method of operation, a tremendous time saver for integration of a large system. The iSeries family includes extremely accurate digital panel meters “DPi” and single loop PID controllers “CNi” that are simple to configure and use, while providing tremendous versatility and a wealth of powerful features.The DPi Series covers a broad selection of transducer and transmitter inputs with 2 input models.The Universal temperature and process instrument (DPi models) handles 10 common types ofthermocouples, multiple RTDs and several process (DC) voltage and current ranges. This model alsofeatures built-in excitation, 24 Vdc @ 25 mA. With its wide choice of signal inputs, this model is an excellent choice for measuring or controlling temperature with a thermocouple, RTD, or 4 to 20 mA transmitter. The strain and process instruments (DPiS models) measure inputs from load cells, pressure transducers, and most any strain gage sensor as well as process voltage and current ranges. The DPiS has built-in 5 or 10 Vdc excitation for bridgetransducers, 5 Vdc @ 40 mA or 10 Vdc @ 60 mA (any excitation voltage between 5 and 24 Vdc is available by special order). This DPiS model supports 4- and 6-wire bridge communications, ratiometric measurements. The DPiS features fast and easy “in process” calibration/scaling of the signal inputs to any engineering units. This model also features 10-point linearization which allows the user to linearize the signal input from extremely nonlinear transducers of all kinds.Programmable Color DisplayThe DPi Series are 1⁄8, 1⁄16 and 1⁄32 DIN digital panel meter featuring the big iSeries color-changing display. The digits are twice the size of typical 1⁄8 DIN panel meters. The iSeries meters feature the only LED displays that can be programmed to change color between GREEN , AMBER , and RED .Embedded internet and serialcommunications featuring optional “embedded Internet” (specify “-EIT” option) the iSeries are the firstinstruments of their kind that connect directly to an Ethernet network and transmit data in standard TCP/IP packets, or even serve Web pages over a LAN or the Internet. The iSeries are also available with serial communications. With the “-C24” option, the user can select from the pushbutton menu between RS232, RS422, and RS485, with straightforward ASCII commands.DPi SeriesU U niversal Inputs U U ser-Friendly, Simple to Configure U H igh Quality U P owerful Features U E xtended 5-Year Warranty U F ree Software Download U T otally Programmable Color Displays U H igh Accuracy: 0.5°C (±0.9°F), 0.03% Reading U B oth RS232 and RS485 Selectable from Menu Available U B uilt-In Excitation U E mbedded Internet Connectivity Optional U R S232 and RS485 Serial Communications Optional U T emperature Stability ±0.04°C/°C RTD and±0.05°C/°C Thermocouple @ 25°C (77°F)U AC or DC Powered Units U R atiometric Mode for Strain Gages U P rogrammableDigital FilterDimensions: mm (inch)CNi16D, shown actual size. Totallyat anysetpointPatentedwith excitation. Models “-EIT” and “-C4EIT”are only offered on DPi8 and DPiS8 models.* 20 to 36 Vdc for DPi8A, DPi16A, -C4EITor -EIT.Ordering Examples:DPi8A,1⁄8 DIN meterwith isolated scalable analog retransmissionof process value. DPi8C,1⁄8 DIN temp/processmeter in compact case, DPi32, 1⁄32 DIN temp/process monitor.C n i S e r i es M o d e l sw i t h C o n tr o l a n da l a r m O ut p u t s,V i s i t O M eG aM-10iSeries ControllersAlso Available!Universal Temperature andProcess Input (DPi/CNi Models)Accuracy: ±0.5°C temp; 0.03% rdg Resolution: 1°/0.1°; 10 µV process Temperature Stability: RTD: 0.04°C/°CTC @ 25°C (77°F): 0.05°C/°C Cold Junction Compensation Process: 50 ppm/°C NMRR: 60 dB CMRR: 120 dBA/D Conversion: Dual slope Reading Rate: 3 samples/s Digital Filter: ProgrammableDisplay: 4-digit 9-segment LED 10.2 mm (0.40"); i32, i16, i16D, i8DV 21 mm (0.83"); i8 10.2 mm (0.40") and 21 mm (0.83"); i8DH RED , GREEN, and AMBER programmable colors for process variable, setpoint and temperature unitsInput Types: Thermocouple, RTD, analog voltage, analog currentThermocouple Lead Resistance: 100 Ω maxThermocouple Types (ITS 90): J, K, T, E, R, S, B, C, N, L (J DIN)RTD Input (ITS 68): 100/500/1000 Ω Pt sensor, 2-, 3- or 4-wire; 0.00385 or 0.00392 curveVoltage Input: 0 to 100 mV, 0 to 1V, 0 to 10 VdcInput Impedance: 10 M Ω for 100 mV 1 M Ω for 1 or 10 VdcCurrent Input: 0 to 20 mA (5 Ω load)Configuration: Single-ended Polarity: UnipolarStep Response: 0.7 sec for 99.9%Decimal Selection:Temperature: None, 0.1Process: None, 0.1, 0.01 or 0.001Setpoint Adjustment: -1999 to 9999 counts Span Adjustment: 0.001 to 9999 countsOffset Adjustment: -1999 to 9999Excitation (Not Included withCommunication): 24 Vdc @ 25 mA (not available for low-power option)Universal Strain and Process Input (DPiS/CNiS Models)Accuracy: 0.03% reading Resolution: 10/1µVTemperature Stability: 50 ppm/°C NMRR: 60 dB CMRR: 120 dBA/D Conversion: Dual slope Reading Rate: 3 samples/s Digital Filter: ProgrammableInput Types: Analog voltage and current Voltage Input: 0 to 100 mVdc, -100 mVdc to 1 Vdc, 0 to 10 VdcInput Impedance: 10 M Ω for 100 mV;1 M Ω for 1V or 10 Vdc Current Input: 0 to 20 mA (5 Ω load)Linearization Points: Up to 10 Configuration: Single-ended Polarity: UnipolarStep Response: 0.7 sec for 99.9%Decimal Selection: None, 0.1, 0.01 or 0.001Setpoint Adjustment: -1999 to 9999 countsSpan Adjustment: 0.001 to 9999 counts Offset Adjustment: -1999 to 9999Excitation (Optional In Place Of Communication): 5 Vdc @ 40 mA;10 Vdc @ 60 mAControlAction: Reverse (heat) or direct (cool)Modes: Time and amplitude proportional control; selectable manual or auto PID, proportional, proportional with integral, proportional with derivative and anti-reset Windup, and on/off Rate: 0 to 399.9 s Reset: 0 to 3999 sCycle Time: 1 to 199 s; set to 0 for on/off Gain: 0.5 to 100% of span; setpoints 1 or 2Damping: 0000 to 0008Soak: 00.00 to 99.59 (HH:MM), or OFF Ramp to Setpoint:00.00 to 99.59 (HH:MM), or OFFAuto Tune: Operator initiated from front panelControl Output 1 and 2Relay: 250 Vac or 30 Vdc @ 3 A (resistive load); configurable for on/off, PID and ramp and soakOutput 1: SPDT, can be configured asalarm 1 outputOutput 2: SPDT, can be configured asalarm 2 outputSSR: ******************.5A (resistive load); continuous DC Pulse: Non-isolated; 10 Vdc @ 20 mA Analog Output (Output 1 Only):Non-isolated, proportional 0 to 10 Vdc or 0 to 20 mA; 500 Ω maxOutput 3 RetransmissionIsolated Analog Voltage and CurrentCurrent: 10 V max @ 20 mA outputVoltage: 20 mA max for 0 to 10 V outputNetwork and Communications Ethernet: Standards compliance IEEE 802.3 10 Base-T Supported Protocols: TCP/IP, ARP, HTTPGET RS232/RS422/RS485: Selectable frommenu; both ASCII and MODBUS protocol selectable from menu; programmable 300 to 19.2 Kb; complete programmable setup capability; program to transmit current display, alarm status, min/max,actual measured input value and statusCommon Specifications (Alli/8, i/16, i/32 DIN)RS485: Addressable from 0 to 199Connection: Screw terminalsAlarm 1 and 2 (Programmable)Type: Same as output 1 and 2Operation: High/low, above/below, band, latch/unlatch, normally open/normally closed and process/deviation; front panel configurationsAnalog Output (Programmable):Non-isolated, retransmission 0 to 10 Vdc or 0 to 20 mA, 500 Ω max (output 1 only); accuracy is ± 1% of FS when following conditions are satisfied: input is not scaled below 1% of input FS, analog output is not scaled below 3% of output FSGeneralPower: 90 to 240 Vac ±10%, 50 to 400 Hz *, 110 to 300 Vdc, equivalent voltage Low Voltage Power Option: 24 Vac **, 12 to 36 Vdc for DPi/CNi/DPiS/CNiS; 20 to 36 Vdc for dual display, ethernet and isolated analog output from qualified safety approved sourceIsolationPower to Input/Output: 2300 Vac per 1 minute testFor Low Voltage Power Option: 1500 Vac per 1 minute test Power to Relay/SSR Output: 2300 Vac per 1 minute testRelay/SSR to Relay/SSR Output: 2300 Vac per 1 minute test RS232/485 to Input/Output: 500 Vac per 1 minute test Environmental Conditions:All Models: 0 to 55°C (32 to 131°F)90% RH non-condensing Dual Display Models:0 to 50°C (32 to 122°F), 90% RHnon-condensing (for UL only) Protection: D Pi/CNi/DPiS/CNiS32, i16, i16D, i8C: NEMA 4X/Type 4 (IP65) front bezel DPi/CNi8, CNi8DH, i8DV: NEMA 1/Type 1 front bezelApprovals: UL, C-UL, CE per 2014/35/EU, FM (temperature units only)Dimensionsi /8 Series: 48 H x 96 W x 127 mm D(1.89 x 3.78 x 5") i/16 Series: 48 H x 48 W x 127 mm D (1.89 x 1.89 x 5")i/32 Series: 25.4 H x 48 W x 127 mm D(1.0 x 1.89 x 5")Panel Cutouti /8 Series: 45 H x 92 mm W(1.772 x 3.622"), 1⁄8 DIN i/16 Series: 45 mm (1.772") square,1⁄16 DINi/32 Series: 22.5 H x 45 mm W(0.886 x 1.772"), 1⁄32 DIN Weight i /8 Series: 295 g (0.65 lb) i/16 Series: 159 g (0.35 lb) i/32 Series: 127 g (0.28 lb)M-11* No CE compliance above 60 Hz. ** Units can be powered safely with 24 Vacpower, but no certification for CE/UL are claimed.。
邮局订阅号:82-946360元/年技术创新电子设计《PLC技术应用200例》您的论文得到两院院士关注1引言作为无线通信系统中的主要模块,射频功放的非线性特性和效率是人们关注的焦点。
射频功放的非线性所引起的频谱扩展会对邻道信号产生干扰,而且带内失真也会增加误码率。
随着新业务的发展(如WCDMA、WIMAX,无线IP网络等,采用MPSK、OFDM等调试方式),具有多载波、宽频带、高峰均比等特性,对于射频功放的线性度提出了更高的要求。
因此,功放预失真器设计的优劣对无线通信系统发射机整体性能的影响是非常大的。
本文详细阐述了射频功放的记忆效应产生的原因及其对数字预失真系统的影响,介绍了可用于描述带记忆效应的功放模型,并提出了可用于带记忆效应功放的数字预失真算法。
通过计算机仿真和实验应用,论证了该算法能有效改善射频功放记忆效应的影响,大大提高了数字预失真系统的准确性和实用性,从而改善无线通信系统发射机的整体性能。
2带记忆效应的数字预失真技术功放的记忆效应主要是由于传输时延、器件特性随温度变化以及器件的频率响应所产生,即功放当前的输出信号不仅与当前的输入信号相关而且与过去的输入信号相关。
对于OFDM等宽频带信号,功放的记忆效应对于信号传输影响变得很大。
发射机功放从本质上来说是一种强记忆效应的功放,对于这种强记忆效应功放,仅仅使用不带记忆效应的预失真器进行补偿的话效果非常有限。
因此,为了更加好的补偿记忆功放的非线性,发射机功放预失真器的设计也必须考虑记忆效应。
2.1功放记忆模型在非线性系统理论中,经常采用Wiener模型、Hammerstein模型、Volterra级数模型建模记忆性非线性系统,论文论述了以上模型的等效性。
Wiener模型和Hammerstein模型的参数最少而且最容易通过数字器件来实现,但是准确有效的识别其模型参数依然非常艰巨的任务。
如图1,Hammerstein模型是由一个无记忆的非线性系统(NL)级联一个线性时不变系统(LTI),Wiener模型其实和Hammerstein模型相似,只不过是把后者的两个子系统交换了。
第 54 卷第 12 期2023 年 12 月中南大学学报(自然科学版)Journal of Central South University (Science and Technology)V ol.54 No.12Dec. 2023模糊PI 控制器与干扰观测器相结合的空间柔性机械臂的转动控制策略上官朝伟1,李小彭1, 2,李泉1,尹猛3(1. 东北大学 机械工程与自动化学院,辽宁 沈阳,110819;2. 宁夏理工学院 机械工程学院,宁夏 石嘴山,753000;3. 中国科学院 深圳先进技术研究院,广东 深圳,518055)摘要:为了减少外部干扰对空间柔性机械臂的系统误差,提高系统的控制精度,提出了一种模糊PI 控制器与干扰观测器相结合的转动控制策略。
首先,采用假设模态法和拉格朗日方法,建立了含有干扰力矩的空间柔性机械臂的初始动力学模型;其次,提出了分别忽略二维变形和忽略非线性项的2种简化动力学模型,并通过仿真分析对比2种简化模型的建模精度;第三,基于极点配置方法和模糊规则设计了模糊PI 控制器,并基于系统的名义模型设计了干扰观测器;最后,通过仿真分析和地面物理样机实验验证了该方法的有效性。
研究结果表明:忽略非线性项的简化模型与初始模型具有相似的建模精度,极大地降低了计算难度,能够代替初始模型进行控制系统的设计;模糊PI 控制器与干扰观测器相结合的转动控制策略能够实时调整控制器参数,观测并补偿干扰力矩引起的系统误差,有效提高系统的控制精度。
关键词:空间柔性机械臂;转动控制策略;简化动力学模型;模糊PI 控制器中图分类号:TH113.1;TP13 文献标志码:A 开放科学(资源服务)标识码(OSID)文章编号:1672-7207(2023)12-4687-12Rotation control strategy for a space-flexible robotic armcombining fuzzy PI controller and disturbance observerSHANGGUAN Chaowei 1, LI Xiaopeng 1, 2, LI Quan 1, YIN Meng 3(1. School of Mechanical Engineering & Automation, Northeastern University, Shenyang 110819, China;2. School of Mechanical Engineering, Ningxia Institute of Science and Technology, Shizuishan 753000, China;3. Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen 518055, China)Abstract: In order to reduce the systematic error of space-flexible robotic arms(SFRA) by external disturbancesand to improve the control accuracy of the system, a rotation control strategy combining fuzzy PI controller and收稿日期: 2023 −01 −15; 修回日期: 2023 −04 −10基金项目(Foundation item):辽宁省应用基础研究计划项目(2023JH2/101300159);宁夏回族自治区自然科学基金资助项目(2023AACO3371) (Project(2023JH2/101300159) supported by the Applied Basic Research Program of Liaoning Province; Project(2023AACO3371) supported by Natural Science Foundation of Ningxia Hui Autonomous Region)通信作者:李小彭,博士,教授,从事机械振动与动力学研究;E-mail :***********DOI: 10.11817/j.issn.1672-7207.2023.12.008引用格式: 上官朝伟, 李小彭, 李泉, 等. 模糊PI 控制器与干扰观测器相结合的空间柔性机械臂的转动控制策略[J]. 中南大学学报(自然科学版), 2023, 54(12): 4687−4698.Citation: SHANGGUAN Chaowei, LI Xiaopeng, LI Quan, et al. Rotation control strategy for a space-flexible robotic arm combining fuzzy PI controller and disturbance observer[J]. Journal of Central South University(Science and Technology), 2023, 54(12): 4687−4698.第 54 卷中南大学学报(自然科学版)disturbance observer was proposed. Firstly, the initial dynamics model of the SFRA containing disturbance torque was established by using the assumed mode method and the Lagrange principle. Secondly, two simplified dynamics models that ignore two-dimensional deformation and ignore non-linear terms were proposed, respectively, and the modeling accuracy of the two simplified models was compared by simulation analysis. Thirdly, a fuzzy PI controller was designed based on the pole placement method and introducing fuzzy rules, and a disturbance observer was designed based on the nominal model of the system. Finally, the effectiveness of the rotation control strategy was verified by simulation analysis and ground physical prototype experiment. The results show that the simplified model ignoring the nonlinear terms has similar modeling accuracy compared with the initial model, which greatly reduces the computational difficulty and can replace the initial model for the design of the control system. The rotational control strategy can adjust the controller parameters in real time, observe and compensate for the system error caused by the disturbance torque, and improve the control accuracy of the system effectively.Key words: space-flexible robotic arms; rotation control strategy; simplified dynamics model; fuzzy PI controller随着机器人技术与航空航天技术的发展,空间柔性机械臂被广泛应用于太空探索作业任务。
Model-Based Synthesis of Nonlinear PI and PIDControllersRaymond A.WrightThe Dow Chemical Company,Midland,MI 48667Costas KravarisDept.of Chemical Engineering,The University of Michigan,Ann Arbor,MI 48109Nikolaos KazantzisDept.of Chemical Engineering,Texas A&M University,College Station,TX 77843PI and PID controllers continue to be popular methods in industrial applications.It is well known that linear PI and PID controllers result from the application of model-based controller design methods to linear first-and second-order systems.It is shown that nonlinear PI and PID controllers result from the application of nonlinear controller design methods to nonlinear first-and second-order systems.As a result,the controllers resulting from nonlinear model-based control theory are put in a con ®enient form,more amenable to industrial implementation.Additionally,the quantities used in the con -troller are useful for monitoring the process and quantifying modeling error.Chemical engineering examples are used to illustrate the resulting control laws.A simulation ex -ample further demonstrates the performance of the nonlinear controllers,as well as their useful process monitoring quantities.IntroductionPI and PID controllers continue to be popular methods for controlling industrial processes,due to their simplicity in im-plementation and understanding.In general,as can be sur-mised from the names,a PI controller possesses proportional and integral action,and a PID controller possesses propor-tional,integral,and derivative action.The standard PI and PID transfer-function forms that are usually presented in Ž.textbooks such as Stephanopoulos,1984areu s 1Ž.s k 1q 1Ž.c ž/e s s Ž.I u s 1Ž.s k 1qq s ,2Ž.c D ž/e s sŽ.I where u is the manipulated input,e is the error signal,s is the Laplace transform variable,and k ,,and are thec I D Correspondence concerning this article should be addressed to R.A.Wright.Current address of C.Kravaris:Dept.of Chemical Engineering,University of Pa-tras,GR-26500Patras,Greece.tunable parameters of the controller.Viewed in its most ba-sic form,these controllers are simply a linear combination of Ž.the 2or 3modes of action.The inclusion of integral action necessarily implies that both controllers are dynamic systems;in a state space representation,there will be a state associ-ated with the controller.In practice,there are several variations of Eqs.1and 2that can be used.For example,the derivative mode of a PID controller may be a numerical derivative,or a filtered value Žto prevent the amplification of noisy signals Stephanopoulos,.1984;Morari and Zafiriou,1989;Ogata,1990.It may be the derivative of the error signal,or the derivative of the mea-sured output,to prevent step changes in the setpoint value˚Žfrom directly effecting the derivative Astromand Witten-¨.mark,1990.The controllers shown in Eqs.1and 2operate solely on the error signal.It is also possible to operate differ-ently on the setpoint value and the measured output.Such a case would be if the derivative was in terms of the measured˚Žoutput only and not based on the error signal Astromand ¨.Wittenmark,1990;Ogata,1990.If the controller is solely de-pendent on the error signal,it can be called an error-feed-back controller,or a one-degree-of-freedom controller.If thecontrol action depends on both the error and the output measurement,it is a mixed error᎐output feedback controller,Ž.or a two-degree-of-freedom controller Kailath,1980.The application of linear model-based controller synthesis methods to linear first-and second-order models can also give rise to a controller of the form of Eq.1or2.As shown in Ž.Ž. Rivera et al.1986,an internal model controller IMC de-rived from a first-order linear model is exactly a linear PI controller,and an IMC controller derived from a linear sec-ond-order model is exactly a linear PID controller.The re-sulting controller,while of the form of Eq.1or Eq.2,has thecontroller gains,k,and,as a function of the modelc I Dparameters and one tunable parameter,which is the closed-loop time constant.Thus,a direct connection can be estab-lished between model parameters and controller tuning.In order to achieve tighter closed-loop control of nonlinear processes,it is natural to generalize Eqs.1or2and develop nonlinear PI and PID controllers.One way would be to add higher-order terms of the error and integral of the error to the control law.Another way suggested in prior work is to make the controller parameters functions of the error Ž.Cheung and Luyben,1980,or PID parameter scheduling Ž.Ž.Rugh,1987,or both Jutan,1989.In general,many differ-ent types of controllers can be classified as nonlinear PI or nonlinear PID,as long as the resulting controller can be shown to possess proportional,integral,and possibly deriva-tive action.There is no particular form that has become stan-dard in the literature.The present work focuses on the development of nonlinear model-based controllers from nonlinear first-and second-order models.This will include nonlinear processes that are exactly first or second order,as well as those processes for which a reasonably accurate low-order model exists and isŽfirst or second order Lindskog and Ljung,1994;Ogunnaike et al.,1994;Balasubramhanya and Doyle,1995;Pearson and.Ogunnaike,1996.In particular,it is shown that the resulting model-based controllers are exactly nonlinear PI and PID controllers,respectively.These results are in the same spiritŽ.as those of Rivera et al.1986,for linear systems.The rela-tion between the model parameters and the controller gains is directly shown,and the tuning of the resulting nonlinear PI or PID controller will be in terms of the closed-loop time constant.The resulting controllers also bring general nonlin-ear controller synthesis to a form that is directly applicable in practice.Furthermore,the terms used in calculating the con-trol action enable the generation and the on-line evaluation of residual quantities that are directly applicable in monitor-ing not only the process but also the magnitude of error in the process model upon which the controller is based.This work begins with the application of nonlinear con-troller synthesis methods to nonlinear first-order models, which results in nonlinear PI controllers.A similar develop-ment,starting with nonlinear second-order models and re-sulting in nonlinear PID controllers,is then presented.Issues arising at the implementation stage,including process moni-toring,on-line measures of model error,and example appli-cations to chemical engineering processes are then discussed. Finally,a CSTR with a nonelementary exothermic reaction is used to demonstrate the closed-loop performance of the pro-posed nonlinear controllers.Model-Based Synthesis of Nonlinear PI Controllers In developing general nonlinear controller synthesis algo-rithms,it is common to begin with a general representation of nonlinear systems.A standard control-affine state-space representation is generally used,and several results are avail-able in the literature for the application of nonlinear model-based controller synthesis methods on models of this form ŽIsidori and Ruberti,1984;Kravaris and Kantor,1990;Be-quette,1991;Kravaris and Arkun,1991;Allgower and Doyle,¨.1996.However,an interpretation of these general results in terms of controller structures that are more commonly used in practice is desirable.In synthesizing nonlinear PI controllers from a nonlinear first-order dynamic model,it is convenient to express the model in terms of a single equation,where the scalar output y is the dependent variable.It is further helpful to use a model where the coefficient of the scalar input u is equal to1.In this work,first-order models of the formdyM y q N y s u3Ž.Ž.Ž.dtwill be used as a starting point.It is important to note that all nonlinear control-affine first-order models with well-defined relative order can be put in the form of Eq.3.In this repre-sentation,the steady-state behavior of the process is cap-Ž.Ž.tured entirely by N y,and the function M y is related solely to the dynamics of the process.These two functions will prove useful in later sections,where using the model for on-line process monitoring is discussed.For the special case where Ž.Ž.M y sr k and N y s y r k,the first-order model becomes the standard linear first-order model expressed in terms of a static gain,k,and a time constant,,which is used as theŽ. basis for deriving linear PI controllers in Rivera et al.1986. Consider the nonlinear first-order process described by Eq. 3and the problem of synthesizing a feedback controller with the following specifications:Ž.1Controller must be first order;Ž.2Controller must possess integral action;Ž.3Controller must induce the linear closed-loop dynamicsdyq y s y,4Ž.cl s pdtwhereis the time constant of the closed-loop system clŽ.tunable parameter.A general nonlinear controller synthesis method,such asŽ.Žglobally linearizing control GLC Kravaris and Chung,1987;.Daoutidis and Kravaris,1992can be used for this purpose. When an open-loop state observer is used in the GLC struc-ture,the resulting controller reduces to a model state-feed-Ž.back controller Kravaris et al.,1994,1998.When applied to Eq.3,this synthesis method results in the following con-Žtroller that meets the specifications just given see the Ap-.pendix for derivationdy eˆsdtcleu s M y q N y,5Ž.Ž.Ž.ˆˆclwhere e s y y y is the error.The state of the controller y is ˆs p the integral of the error scaled by the closed-loop time con-stant .The controller given by Eq.5thus has integral ac-cl tion,and since the error appears explicitly in the calculation of the manipulated input,it also has proportional action.Since the only input in Eq.5is the error signal,this con-troller is a one-degree-of-freedom nonlinear PI controller.Before proceeding,it is important to note two other as-Ž.pects of the state of the controller Eq.5.First,from Eq.4,the desirable closed-loop input ᎐output behavior isy y ydy s p s .6Ž.dt clThus,the controller state y represents the precalculated evo-ˆlution of the output in closed-loop.Additionally,the controlŽ.law Eq.5forces y to match with y so that the closed-loop ˆdynamics follows Eq.4.Notice that this happens after cancel-lation at the process modes.Indeed,combining Eq.3with Eq.5results indy dy ˆM y q N y s M y q N y ,7Ž.Ž.Ž.Ž.Ž.ˆˆdtdtfrom which y will asymptotically approach y ,with the speedˆŽ.of the dynamics Eq.3,as long as the dynamics Eq.3is stable.The application of the same nonlinear controller synthesis method to a linear first-order process in standard form re-sults in the linear controlleru s 1Ž.s1q,8Ž.ž/e s k sŽ.clwhen put in transfer-function form.By comparing Eq.8with Eq.1,it can clearly be seen that this is a standard linear one-degree-of-freedom PI controller with gain k s r k c cl and reset time s .The resulting controller,Eq.8,is iden-I Ž.tical to the one derived by Rivera et al.1986using the IMC method.If it is desired that the location of the zero-pole cancella-tion be arbitrarily assigned instead of having it at the process mode,an alternative solution to the posed synthesis problem can be obtained.This can be accomplished using the GLC Žsynthesis method Kravaris and Chung,1987;Daoutidis and .ŽKravaris,1992and results in the following controller see .the Appendix for derivation dy eˆsdtcl e y y y ˆu s M y qq N y ,9Ž.Ž.Ž.clcwhich has two tunable parameters,and .The state ofcl c the controller represented by Eq.9is exactly the same as the state of the controller represented by Eq.5;it is therefore proportional to the integral of the error and represents the precalculated evolution of the output that the controller is trying to enforce.The controller clearly has both integral and proportional action.Notice,however,that both the error and the measured output directly enter the calculation of the ma-nipulated input.Therefore,this control law is mixed error-output feedback,or a two-degree-of-freedom nonlinear PI controller.With the controller given by Eq.9,the closed-loop system follows the dynamicsy y ydy ˆs p sdt cl y y ydy y y y ˆs p sq,10Ž.dtclcfrom whichd 1y y y sy y y y ,11Ž.Ž.Ž.ˆˆdtcand therefore y will asymptotically approach y with time ˆconstant .Thus,the tunable parameter measures the c c ‘‘hidden dynamics ’’of the closed-loop system,or,stated an-other way,the closed-loop system has a zero-pole cancella-tion at y 1r.c The application of the same nonlinear controller synthesis method to a linear first-order process in standard form re-sults in the linear controller111u s s1qe s yyy s ,12Ž.Ž.Ž.Ž.ž/ž/k skclc cwhen put in transfer function form.This would be exactly the same result as if one were to design a controller via polyno-Žmial equations and solve a Diophantine equation Kailath,.1980for the given specifications of closed-loop input ᎐output behavior and zero-pole cancellation.The two-degree-of-free-dom controller has proportional and integral action in the error,but only proportional action in y .When the process is unstable,the P -action in y can be interpreted as a prestabi-lizing inner loop that shifts the pole to y 1r,and the PI-ac-c tion in the error as an outer loop that enforces the desired trajectory.Notice also that if is selected to equal ,the c Ž.controller Eq.12becomes identically equal to that of Eq.8.It has been shown in this section that if a general nonlinear controller synthesis method is applied to a nonlinear first-order process model,a nonlinear PI controller will naturally result.A slight variation of the method can yield either a one-degree-of-freedom controller,where a zero-pole cancel-lation will occur at the process mode,or a two-degree-of-freedom controller,where the zero-pole cancellation can be arbitrarily assigned.The closed-loop time constant is a tun-able parameter,which may be selected in a manner con-sistent with standard performance r robustness trade-offs.The model parameters,or nonlinear functions,will automatically appear in the control law in a physically meaningful way.The resulting nonlinear controllers are directly linked to the pro-cess,yet are easily understandable in the context of standard linear PI controllers and can be implemented within the same framework.These points and the applicability of the con-troller quantities for process monitoring will be discussed in the context of more specific chemical engineering processes in a later section.Model-Based Synthesis of Nonlinear PIDControllersWhile nonlinear PI controllers arise naturally from nonlin-ear first-order process models,in this section it will be shown that nonlinear PID controllers arise naturally from nonlinear second-order process models of relative order 2.A general second-order nonlinear control-affine model of relative order 2can always be expressed in terms of a second-order differ-ential equation of the formdy d 2y dy M y ,q N y ,s u 13Ž.2ž/ž/dtdtdt ŽŽ..ŽŽ..The functions M y ,dy r dt and N y ,dy r dt can most eas-Žily be calculated by putting the system in normal form Isidori,.1989;Nijmeijer and van der Schaft,1990through a coordi-nate transformation,converting the normal form into a sec-ond-order differential equation,and rearranging the coeffi-cients.Notice that the steady-state behavior is captured by Ž.N y ,0and that the part of the model described by ŽŽ..M y dy r dt is solely related to the dynamics of the process.ŽŽ..2For the special case where M y ,dy r dt s r k anddyy 2dyN y ,s q ,ž/dt k k dtthe second-order model becomes the standard linearsecond-order model expressed in terms of a static gain k ,a time constant ,and a damping factor ,which is used as a Ž.basis for deriving linear PID controllers in Rivera et al.1986.Consider the nonlinear second-order process described by Eq.13and the problem of synthesizing a feedback controller with the following specifications:Ž.1Controller must be second order.Ž.2Controller must possess integral action.Ž.3Controller must induce the linear closed-loop dynamicsd 2y dy UUq q q y s y 14Ž.Ž.cl cl cl cl s p2dtdt where and Uare the closed-loop time constantscl cl Ž.Utunable parameters .In the limit as ™0,the closed-loop cl dynamics in Eq.14will approach the one described by Eq.4.This limiting case will also be considered and will lead to ideal derivative action.A solution to the posed problem can be derived using the GLC synthesis method in the form of the model state-feed-Ž.back structure Kravaris et al.,1994,1998.When applied to ŽEq.13,this structure results in the following controller see.the Appendix for derivation dy ˆs sˆdtUds eˆcl cls y s 15Ž.ˆUU q dtq cl cl cl cley sˆUq cl clu s M y ,s q N y ,s .Ž.Ž.ˆˆˆˆUcl clUq cl clOne state of the controller s represents the result of filteringˆŽU.the time-scaled error e r q with filter time constant cl clŽU .ŽU.r q .The other state of the controller y is ex-ˆcl cl cl cl actly the integral of s .Therefore,y is the integral of the ˆˆfiltered error scaled by the sum of the closed-loop time con-stants q U.Furthermore,from Eq.14,the desirable cl clclosed-loop dynamics of the output followsdy s s dtU y y ydss p cl cls y s .16Ž.UUq dtq cl cl cl clThus,the controller states y and s represent the precalcu-ˆˆŽ.lated evolution of the output y and its derivative s s dy r dt ,which the controller is trying to enforce.The controller given by Eq.15has integral and derivative action,and since the error appears explicitly in the calculation of the manipulated input,it also has proportional action.The only input into Eq.15is the error signal,therefore this controller is a one-de-gree-of-freedom nonlinear PID controller.It is interesting to examine the limiting case U™0.In this clŽ.case,the time constant of the second-state equation Eq.15ŽU .ŽU .r q ™0,and therefore s ™e r .Moreover,ˆcl cl cl cl cl eUds 1deˆcl cl y ss™,ˆUž/ž/q q dtdtcl clcl clcl Ž.and the controller Eq.15tends tody eˆs17Ž.dtcle1deeu s M y ,q N y ,,ˆˆž/ž/dtclcl clwhich is an ideal one-degree-of-freedom nonlinear PID con-troller,as opposed to Eq.15,which has filtered derivative action.Note that with the controller represented in Eq.15or Eq.17,the requested closed-loop input r output behavior in Eq.14or Eq.4is obtained after cancellations at the processmodes.For example,combining Eq.17with Eq.13results indy d 2y dy dy d 2y ˆˆM y ,q N y ,s M y ,ˆ22ž/ž/ž/dtdtdt dtdtdy ˆq N y ,,18Ž.ˆž/dtfrom which y will asymptotically approach y ,with the speedˆof dynamics of Eq.13,as long as Eq.13is stable.The application of the same nonlinear controller synthesis method to a linear second-order process in standard form results in the controlleru s 21Ž.s1qqs19Ž.ž/e s k 2s2Ž.clwhen put in transfer-function form.By comparing Eq.19with Eq.2it can clearly be seen that this is a standard linear one-Ž.degree-of-freedom PID controller with gain k s 2r k ,c cl reset time s 2,and rate time s r 2.The resulting I D Ž.controller Eq.19is identical to the one derived by Rivera et Ž.al.1986using the IMC method.If it is desired to arbitrarily assign the location of the zero-pole cancellations instead of having them at the process modes,an alternative solution to the posed synthesis problem can be obtained.This can be accomplished using the GLC Žsynthesis method Kravaris and Chung,1987;Daoutidis and .ŽKravaris,1992and results in the following controller see .the Appendix for derivation dy eˆs20Ž.dtcldy 1deq e dy y y y ˆca cb u s M y ,qy q½5ž/ž/dtdtdtcl ca cbclca cbdy q N y ,,ž/dtwith tunable parameters ,,and .Comparing Eq.20cl ca cb to Eq.17,it can clearly be seen that both controllers have ideal derivative action and the same state y ,which is a time-ˆscaled integral of the error.The manipulated input calcu-lated in Eq.20depends directly on both the error and mea-sured output.This controller is clearly mixed error-output feedback,or a two-degree-of-freedom nonlinear PID con-troller.However,control action is calculated differently in Eq.20than it is in Eq.17,and this impacts the behavior of Ž.the closed-loop system.With the controller Eq.20applied to Eq.13,the closed-loop system follows the dynamicsy y ydy ˆs p s 21Ž.dtcl2d y y y y y yd y 1q dy y y y Ž.ˆs p s p ca cb sqyq2ž/dtdtdt cl ca cbclca cbŽ.w Ž.x .Substituting y y y r by dy r dt and 1r d y y y r dt by ˆs p cl cl s p d 2y r dt 2in Eq.21,it follows thatˆd 2y y y q d y y y y y y Ž.Ž.ˆˆˆca cb qqs 0,22Ž.2dtdt ca cbca cband therefore y will asymptotically approach y with time ˆconstants and .Thus,the tunable parameters and ca cb ca account for the ‘‘hidden dynamics ’’of the closed-loop sys-cb tem;the closed-loop system has zero-pole cancellations aty 1rand y 1r .ca cb The application of the same nonlinear controller synthesis method to a linear second-order process in standard form results in the linear controller 2q 1ca cb u s sqq s e s Ž.Ž.ž/k s cl ca cbca cb 211q 2ca cb yyq ys y s 23Ž.Ž.2ž/kca cbca cbwhen put in transfer function form.This would be exactly thesame result as if one were to design a controller via polyno-Žmial equations and solve a Diophantine equation Kailath,.1980for the given specifications of closed-loop input ᎐output behavior and zero-pole cancellations.The two-degree-of-freedom controller has proportional,integral,and derivative action in the error,but only proportional and derivative ac-tion in y .When the process is unstable,the PD action in y can be interpreted as a prestabilizing inner loop that shiftsthe poles to y 1rand y 1r and the PID action in the ca cb error as an outer loop that enforces the desired trajectory.Notice also,that if and are chosen so that s 2c a cb c a cb Ž.and q s 2,the controller Eq.23becomes identi-ca cb cally equal to Eq.19.It has been shown in this section that if a general nonlinear controller synthesis method is applied to a nonlinear second-order process model of relative order 2,a nonlinear PID con-troller will result.A slight variation on the method can yield either a one-degree-of-freedom controller,where the zero-pole cancellations will occur at the process modes,or a two-degree-of-freedom controller,where the zero-pole cancella-tions may be arbitrarily assigned.The closed-loop time con-stant is a tunable parameter,which can be selected in a man-ner consistent with standard performance r robustness trade-offs.The model parameters,or nonlinear functions,will au-tomatically appear in the control law in a physically meaning-ful way.The resulting nonlinear controllers are directly linked to the process,yet easily understandable in the context of standard linear PID controllers and can be implemented within the same framework.These points and the applicabil-ity of the controller quantities for process monitoring will be discussed in the next section in the context of more specific chemical engineering processes.A Practical Interpretation of Results and Examples of Applications to Chemical ProcessesAs with all model-based controllers,their performance in the presence of modeling error,or in other words how accu-rate the models need to be for good closed-loop performanceis naturally a concern.Local robustness results are available Žin the literature Kravaris and Palanki,1988;Byrnes et al.,.1997for general nonlinear input ᎐output linearization meth-ods.Since these methods were used in deriving the con-trollers in the previous sections,the controllers obviously in-herit these results.From the specific form of these con-trollers,however,it is straightforward to see how modeling error will be rejected.Relevant quantities that can be used on-line in a simple process-monitoring scheme,or as a mea-sure of the accuracy of the model upon which the controller is based,are inherent in the controller structure.Consider the case of a first-order nonlinear process,which is not exactly known,and is represented bydy M y q N y s u 24Ž.Ž.Ž.p p dt dy M y q N y s u ,25Ž.Ž.Ž.m m dtwhere the subscript p denotes the true process and the sub-script m denotes the model of the process.The closed-loopsystem under the one-degree-of-freedom nonlinear PI con-Ž.troller Eq.5isy y ydy ˆs p s dtcl y y y N y y N y dy M y Ž.Ž.Ž.ˆˆs p m p m sq.26Ž.dt M y M y Ž.Ž.p clp When the closed-loop system is at steady state,the followingrelations will holdy s y s s pu s N y s N y ,27Ž.Ž.Ž.ˆs m s p s p where the subscript s denotes a steady-state value.A few keyquantities can be used to quantify the difference between the model and the process or whether an unmeasured disturb-ance has entered the process.The state of all the controllers developed in this work y is also an estimate of the measured ˆoutput y .In the absence of modeling error,y will track y .ˆThe difference y y y is a measure of the error in terms of the ˆŽ.Ž.process output.Tracking the difference N y y N y pro-ˆm m vides useful information in quantifying modeling error in terms of the process input.At steady state,the controller Ž.forces N y to equal u ,and the difference between these ˆm Ž.quantities and N y is exactly the model error in the m steady-state part of the process model.ŽIf the two-degree-of-freedom nonlinear PI controller Eq..9is used,the closed-loop system is y y ydy ˆs p s dt cl y y yN y y N y dy M y y y y Ž.Ž.Ž.ˆs p m p m sqq.28Ž.dt M y M y Ž.Ž.p clcp When the closed-loop system is at steady state,the following relations will holdy s y s s py y y ˆs s u s N y q M y s N y .29Ž.Ž.Ž.Ž.s m s m s p s cIn this case,since the location of the zero-pole cancellation istunable,the speed with which modeling error is rejected,as well as the difference y y y ,will be different than the one-ˆdegree-of-freedom controller case.The state of the controller is still an estimate of the measured output,but the difference Ž.y y y will depend on .Tracking N y with u will provide ˆc m exactly the same useful information in quantifying modeling error as it did with the one-degree-of-freedom controller.The Ž.difference N y y u is exactly the modeling error in the m s s steady-state part of the model.This discussion has focused entirely on first-order systems and the use of nonlinear PI controllers.The analysis for sec-ond-order systems and nonlinear PID controllers is essen-tially the same and will be omitted here for brevity.The quantities that are useful to track on-line will be the same,Ž.Ž.only using N ؒ,0in place of N ؒ.The use of these quanti-ties will be demonstrated for PID controllers in the simulated example in the next section.Another concern with the implementation of model-based controllers is the degree to which controller code can be standardized to allow for minimum long-term maintenance costs.The form in which controllers were derived in this work is a good form for direct implementation.The calculation of the state variable is straightforward and very similar to the calculation of the integral in a standard linear PI or PID con-troller.The calculation of the manipulated input remains the same for each controller,in terms of the M and N functions.These two functions are all that vary as the model is changed.Visualizing these two functions as subroutines means that changing a model is as simple as replacing a subroutine.Moreover,the rest of the controller will be very similar to the standard linear controllers that are usually prevalent in in-dustrial plants.Finally,the M and N functions are directly tied to a model of the process,which can be included in the documentation for the controller.These points will be fur-ther illustrated in a series of examples.Example 1.Consider a batch reactor with negligible jacket dynamics and an irreversible,zero-order reaction,A ™B .An energy balance around the reactor yieldsdT UAk e y E r RT y ⌬H Ž.0sT y T q.30Ž.Ž.j dtc Vc Vp p The objective is to control the reactor temperature,T ,bymanipulating the jacket temperature,T .Either the one-de-j Ž.gree-of-freedom nonlinear PI Eq.5,or the two-degree-of-Ž.freedom nonlinear PI Eq.9can be applied.For this exam-。