Department of Electrical and Computer Engineering

Slides:



Advertisements
Similar presentations
Representation of Hysteresis with Return Point Memory: Expanding the Operator Basis Gary Friedman Department of Electrical and Computer Engineering Drexel.
Advertisements

Lect.3 Modeling in The Time Domain Basil Hamed
A New Hysteretic Reactor Model for Transformer Energization Applications Title: By : Afshin Rezaei-Zare & Reza Iravani University of Toronto June 2011.
Information Processing & Digital Systems COE 202 Digital Logic Design Dr. Aiman El-Maleh College of Computer Sciences and Engineering King Fahd University.
Presenter: Yufan Liu November 17th,
Parametric Inference.
1 A Dynamic Model for Magnetostrictive Hysteresis Xiaobo Tan, John S. Baras, and P. S. Krishnaprasad Institute for Systems Research and Department of Electrical.
Detection of multi-stability in biological feedback systems George J. Pappas University of Pennsylvania Philadelphia, USA.
AP Statistics Section 10.2 A CI for Population Mean When is Unknown.
©2003/04 Alessandro Bogliolo Background Information theory Probability theory Algorithms.
When a ferromagnetic material is magnetized in one direction, it will not relax back to zero magnetization when the imposed magnetizing field is removed.
Lecture 35 Numerical Analysis. Chapter 7 Ordinary Differential Equations.
Gaussian process modelling
Mihai Octavian POPESCU, Claudia POPESCU Faculty of Electrical Engineering UPB Electrical Engineering- Ideas for the Future.
A Shaft Sensorless Control for PMSM Using Direct Neural Network Adaptive Observer Authors: Guo Qingding Luo Ruifu Wang Limei IEEE IECON 22 nd International.
A Comparison of a Mean Field Theoretic Approach to Ferromagnetism with Experimental Results Patrick Yarbrough- Department of Physics and Engineering The.
Infinite Series Copyright © Cengage Learning. All rights reserved.
Functions. Quick Review What you’ll learn about Numeric Models Algebraic Models Graphic Models The Zero Factor Property Problem Solving Grapher.
difficult if we consider Didn’t you say it’s a very
Taylor Series Mika Seppälä. Mika Seppälä: Taylor Polynomials Approximating Functions It is often desirable to approximate functions with simpler functions.
1 CS 430/536 Computer Graphics I Curve Drawing Algorithms Week 4, Lecture 8 David Breen, William Regli and Maxim Peysakhov Geometric and Intelligent Computing.
Distribution of the Sample Means
ELECTRICAL ENGINEERING: PRINCIPLES AND APPLICATIONS, Fourth Edition, by Allan R. Hambley, ©2008 Pearson Education, Inc. Lecture 21 Magnetic Circuits, Materials.
Lecture 18 Chapter 32 Outline Gauss Law for Mag Field Maxwell extension of Ampere’s Law Displacement Current Spin/ Orbital Mag Dipole Moment Magnetic Properties.
Welcome Back Scientists! Today: 1. Return Electromagnets Inquiry Scores 2. Discuss the Revision Process 3. Interactions between permanent and Electromagnets:
Welcome Scientists Today: Complete Building a Motor Activity Motors Vs. Generators Electricity and Magnetism Mind-Map.
Simulation and Experimental Verification of Model Based Opto-Electronic Automation Drexel University Department of Electrical and Computer Engineering.
A theory of reverse engineering N.Y. Louis Lee (1) & P.N. Johnson-Laird (2) (1)Department of Educational Psychology, Faculty of Education, The Chinese.
Lecture 8 1 Ampere’s Law in Magnetic Media Ampere’s law in differential form in free space: Ampere’s law in differential form in free space: Ampere’s law.
Eeng Chapter 5 AM, FM, and Digital Modulated Systems  Phase Modulation (PM)  Frequency Modulation (FM)  Generation of PM and FM  Spectrum of.
Keywords (ordinary/partial) differencial equation ( 常 / 偏 ) 微分方程 difference equation 差分方程 initial-value problem 初值问题 convex 凸的 concave 凹的 perturbed problem.
Dr.Mohammed abdulrazzaq
Sampling and Sampling Distributions
Section 8.2: The Sampling Distribution of a Sample Mean
CS 9633 Machine Learning Support Vector Machines
ECE 6382 Notes 6 Power Series Representations Fall 2016
EEE4176 Applications of Digital Signal Processing
Copyright © Cengage Learning. All rights reserved.
Boundary Element Analysis of Systems Using Interval Methods
Tirza Routtenberg Dept. of ECE, Ben-Gurion University of the Negev
CHAPTER VI BLOCK DIAGRAMS AND LINEARIZATION
Notes for Analysis Et/Wi
CT-321 Digital Signal Processing
Class Notes 9: Power Series (1/3)
Taylor Polynomials & Approximation (9.7)
SAT-Based Area Recovery in Technology Mapping
The Curve Merger (Dvir & Widgerson, 2008)
Reinforcement Learning with Partially Known World Dynamics
The Normal Probability Distribution Summary
Sequences and Series 4.7 & 8 Standard: MM2A3d Students will explore arithmetic sequences and various ways of computing their sums. Standard: MM2A3e Students.
Darko Simonovic Department of Materials Science & Engineering
Quantum mechanics II Winter 2011
Section 2-1: Functions and Relations
AN INTRODUCTION TO COMPUTER GRAPHICS Subject: Computer Graphics Lecture No: 01 Batch: 16BS(Information Technology)
Homework 1: Electrical System
5.3 Higher-Order Taylor Methods
Lecture 3 Sorting and Selection
CONTROL SYSTEM AN INTRODUCTION.
Introduction to Radial Basis Function Networks
Numerical Analysis Lecture 2.
ELEC207 Linear Integrated Circuits
Recursively Adapted Radial Basis Function Networks and its Relationship to Resource Allocating Networks and Online Kernel Learning Weifeng Liu, Puskal.
Wellcome Centre for Neuroimaging at UCL
INTERSYMBOL INTERFERENCE (ISI)
Sampling Distributions (§ )
Signals and Systems Lecture 2
Clustering.
The Selection Problem.
Copyright © Cengage Learning. All rights reserved.
Ginzburg-Landau theory
Presentation transcript:

Department of Electrical and Computer Engineering Representation of Hysteresis with Return Point Memory: Expanding the Operator Basis Gary Friedman Department of Electrical and Computer Engineering Drexel University

Hysteresis forms M Dave H Dint Form most frequently associated with hysteresis: magnets Ratchets, swimming, molecular motors, etc.

Return Point (wiping-out) Memory The internal state variables return when the input returns to its previous extremum. Experimentally observed in: magnetic materials, superconductors, piezo-electric materials, shape memory alloys, absorption Also found in micro-models: Random Field Ising Models (with positive interactions), Sherrington - Kirkpatrick type models, models of domain motion in random potential,

How can we represent any hysteresis with wipe-out memory in general How can we represent any hysteresis with wipe-out memory in general? Can we approximate any hysteresis with wipe-out memory? Preisach model represents some hysteresis with wipe-out memory because each bistable relay has wipe-out memory. It also has the property of Congruency which is an additional restriction

Congruency Any higher order reversal curve is congruent to the first order reversal curve. All loops bounded between the same input values are congruent. Higher order reversal curves could, in general, deviate from first order reversal curve. These deviations can not be accounted for in the Preisach model.

Examples of systems with Return Point Memory, but without Congruency Mean-field models in physics Interacting networks of economic agents Theorem: as long as interactions are positive, such systems have RPM (Jim Senthna, Karin Dahmen) Problem: Not clear if or when model unique model parameters can be identified using macroscopic observations

Mapping of history into output of the model (Martin Brokate) Any hysteresis with wipe-out memory can be represented by a mapping of the interface function into the output Interface function represents the state of hysteresis transducer with wipe-out memory.

How can an approximation be devised? Assume both, the given hysteresis transducer and the approximation we seek are sufficiently smooth mappings of history into the output

Nth order approximation

Building Nth order approximation “Matryoshka” threshold set Key point: as long as operators are functions of elementary rectangular loop operator, the system retains Return Point Memory

Higher order elementary operators Second order elementary operator example

Why use only “Matryoshka” threshold sets? Non-”Matryoshka” operators can be reduced to lower order “Matryoshka” operators

Nth order Preisach model Loops appear only after Nth order reversal. Reversal curves following that are congruent to Nth order reversal as long they have the same preceding set of first N reversals

Nth order approximation Due to second order Preisach model Due to first order Preisach model

Conclusion As long as the hysteretic system with RPM is a “smooth” mapping of history, it is possible to approximate it with arbitrary accuracy on the basis of higher order rectangular hysteresis operators. It is a sort of analog to Taylor series expansion of functions; Nth order approximation satisfies Nth order congruency property which is much less restrictive than the first order congruency property