Elements of Applied Bifurcation Theory

Size: px
Start display at page:

Download "Elements of Applied Bifurcation Theory"

Transcription

1 Yuri A. Kuznetsov Elements of Applied Bifurcation Theory Third Edition With 251 Illustrations Springer

2 Introduction to Dynamical Systems Definition of a dynamical system State space Time Evolution operator Definition of a dynamical system Orbits and phase portraits Invariant sets Definition and types Smale horseshoe Stability of invariant sets Differential equations and dynamical systems Poincare maps Time-shift maps Poincare map and stability of cycles Poincare map for periodically forced systems Exercises Appendix A: Infinite-dimensional dynamical systems defined by reaction-diffusion equations Appendix B: Bibliographical notes 36 Topological Equivalence, Bifurcations, and Structural Stability of Dynamical Systems Equivalence of dynamical systems Topological classification of generic equilibria and fixed points Hyperbolic equilibria in continuous-time systems Hyperbolic fixed points in discrete-time systems Hyperbolic limit cycles Bifurcations and bifurcation diagrams Topological normal forms for bifurcations Structural stability 67

3 XVIII 2.6 Exercises Appendix: Bibliographical notes 75 3 One-Parameter Bifurcations of Equilibria in Continuous- Time Dynamical Systems Simplest bifurcation conditions The normal form of the fold bifurcation Generic fold bifurcation The normal form of the Hopf bifurcation Generic Hopf bifurcation Exercises Appendix A: Proof of Lemma Appendix B: Poincare normal forms Appendix C: Bibliographical notes One-Parameter Bifurcations of Fixed Points in Discrete-Time Dynamical Systems Simplest bifurcation conditions The normal form of the fold bifurcation Generic fold bifurcation The normal form of the flip bifurcation Generic flip bifurcation The "normal form" of the Neimark-Sacker bifurcation Generic Neimark-Sacker bifurcation Exercises Appendix A: Feigenbaum's universality Appendix B: Proof of Lemma Appendix C: Bibliographical notes Bifurcations of Equilibria and Periodic Orbits in n-dimensional Dynamical Systems Center manifold theorems Center manifolds in continuous-time systems Center manifolds in discrete-time systems Center manifolds in parameter-dependent systems Bifurcations of limit cycles Computation of center manifolds Restricted normalized equations for ODEs Restricted normalized equations for maps Exercises Appendix A: Hopf bifurcation in reaction-diffusion systems Appendix B: Bibliographical notes 194

4 XIX 6 Bifurcations of Orbits Homoclinic and Heteroclinic to Hyperbolic Equilibria 195, 6.1 Homoclinic and heteroclinic orbits Andronov-Leontovich theorem Homoclinic bifurcations in three-dimensional systems: Shil'nikov theorems Homoclinic bifurcations in n-dimensional systems Regular homoclinic orbits: Melnikov integral Homoclinic center manifolds Generic homoclinic bifurcations inr Exercises Appendix A: Focus-focus homoclinic bifurcation in four-dimensional systems Appendix B: Bibliographical notes Other One-Parameter Bifurcations in Continuous-Time Dynamical Systems Codim 1 bifurcations of homoclinic orbits to nonhyperbolic equilibria Saddle-node homoclinic bifurcation on the plane Saddle-node and saddle-saddle homoclinic bifurcations in E Bifurcations of orbits homoclinic to limit cycles Nontransversal homoclinic orbit to a hyperbolic cycle Homoclinic orbits to a nonhyperbolic limit cycle Bifurcations on invariant tori Reduction to a Poincare map Rotation number and orbit structure Structural stability and bifurcations Phase locking near a Neimark-Sacker bifurcation: Arnold tongues Bifurcations in symmetric systems General properties of symmetric systems Z2-equivariant systems Codim 1 bifurcations of equilibria in Z2-equivariant systems Codim 1 bifurcations of cycles in Z2-equivariant systems Exercises Appendix: Bibliographical notes Two-Parameter Bifurcations of Equilibria in Continuous- Time Dynamical Systems List of codim 2 bifurcations of equilibria Codim 1 bifurcation curves Codim 2 bifurcation points 299

5 XX 8.2 Cusp bifurcation ' Normal form derivation Bifurcation diagram of the normal form Effect of higher-order terms Bautin (generalized Hopf) bifurcation Normal form derivation Bifurcation diagram of the normal form Effect of higher-order terms Bogdanov-Takens (double-zero) bifurcation Normal form derivation Bifurcation diagram of the normal form Effect of higher-order terms Fold-Hopf bifurcation Derivation of the normal form Bifurcation diagram of the truncated normal form Effect of higher-order terms Hopf-Hopf bifurcation Derivation of the normal form Bifurcation diagram of the truncated normal form Effect of higher-order terms Critical normal forms for n-dimensional systems The method Cusp bifurcation Bautin bifurcation Bogdanov-Takens bifurcation Fold-Hopf bifurcation Hopf-Hopf bifurcation Exercises Appendix A: Limit cycles and homoclinic orbits of Bogdanov normal form Appendix B: Bibliographical notes Two-Parameter Bifurcations of Fixed Points in Discrete-Time Dynamical Systems List of codim 2 bifurcations of fixed points Cusp bifurcation Generalized flip bifurcation Chenciner (generalized Neimark-Sacker) bifurcation Strong resonances Approximation by a flow :1 resonance :2 resonance :3 resonance :4 resonance Fold-flip bifurcation 466

6 XXI 9.7 Critical normal forms for n-dimensional maps Cusp Generalized flip Chenciner bifurcation Resonance 1: Resonance 1: Resonance 1: Resonance 1: Fold-flip Codim 2 bifurcations of limit cycles Exercises Appendix: Bibliographical notes Numerical Analysis of Bifurcations Numerical analysis at fixed parameter values Equilibrium location Modified Newton's methods Equilibrium analysis Location of limit cycles One-parameter bifurcation analysis Continuation of equilibria and cycles Detection and location of codim 1 bifurcations Analysis of codim 1 bifurcations Branching points Two-parameter bifurcation analysis Continuation of codim 1 bifurcations of equilibria and fixed points Continuation of codim 1 limit cycle bifurcations Continuation of codim 1 homoclinic orbits Detection, location, and analysis of codim 2 bifurcations Continuation strategy Exercises Appendix A: Convergence theorems for Newton methods Appendix B: Bialternate matrix product Appendix C: Detection of codim 2 homoclinic bifurcations Singularities detectable via eigenvalues Orbit and inclination flips Singularities along saddle-node homoclinic curves Appendix D: Bibliographical notes 581 A Basic Notions from Algebra, Analysis, and Geometry 587 A.I Algebra >. 587 A.1.1 Matrices 587 A. 1.2 Vector spaces and linear transformations 589 A.1.3 Eigenvectors and eigenvalues 590

7 XXII A.1.4 Invariant subspaces, generalized eigenvectors, and Jordan normal form 591 A.I.5 Fredholm Alternative Theorem 592 A.1.6 Groups 593 A.2 Analysis 593 A.2.1 Implicit and Inverse Function Theorems 593 A.2.2 Taylor expansion 594 A.2.3 Metric, normed, and other spaces 595 A.3 Geometry 596 A.3.1 Sets 596 A.3.2 Maps 597 A.3.3 Manifolds 597 References 599 Index 619

Elements of Applied Bifurcation Theory

Elements of Applied Bifurcation Theory Yuri A. Kuznetsov Elements of Applied Bifurcation Theory Second Edition With 251 Illustrations Springer Preface to the Second Edition Preface to the First Edition vii ix 1 Introduction to Dynamical Systems

More information

Elements of Applied Bifurcation Theory

Elements of Applied Bifurcation Theory Yuri A. Kuznetsov Elements of Applied Bifurcation Theory Third Edition With 251 Illustrations Springer Yuri A. Kuznetsov Department of Mathematics Utrecht University Budapestlaan 6 3584 CD Utrecht The

More information

BIFURCATION PHENOMENA Lecture 4: Bifurcations in n-dimensional ODEs

BIFURCATION PHENOMENA Lecture 4: Bifurcations in n-dimensional ODEs BIFURCATION PHENOMENA Lecture 4: Bifurcations in n-dimensional ODEs Yuri A. Kuznetsov August, 2010 Contents 1. Solutions and orbits: equilibria cycles connecting orbits compact invariant manifolds strange

More information

Introduction to Applied Nonlinear Dynamical Systems and Chaos

Introduction to Applied Nonlinear Dynamical Systems and Chaos Stephen Wiggins Introduction to Applied Nonlinear Dynamical Systems and Chaos Second Edition With 250 Figures 4jj Springer I Series Preface v L I Preface to the Second Edition vii Introduction 1 1 Equilibrium

More information

NBA Lecture 1. Simplest bifurcations in n-dimensional ODEs. Yu.A. Kuznetsov (Utrecht University, NL) March 14, 2011

NBA Lecture 1. Simplest bifurcations in n-dimensional ODEs. Yu.A. Kuznetsov (Utrecht University, NL) March 14, 2011 NBA Lecture 1 Simplest bifurcations in n-dimensional ODEs Yu.A. Kuznetsov (Utrecht University, NL) March 14, 2011 Contents 1. Solutions and orbits: equilibria cycles connecting orbits other invariant sets

More information

DYNAMICAL SYSTEMS. I Clark: Robinson. Stability, Symbolic Dynamics, and Chaos. CRC Press Boca Raton Ann Arbor London Tokyo

DYNAMICAL SYSTEMS. I Clark: Robinson. Stability, Symbolic Dynamics, and Chaos. CRC Press Boca Raton Ann Arbor London Tokyo DYNAMICAL SYSTEMS Stability, Symbolic Dynamics, and Chaos I Clark: Robinson CRC Press Boca Raton Ann Arbor London Tokyo Contents Chapter I. Introduction 1 1.1 Population Growth Models, One Population 2

More information

Lecture 5. Numerical continuation of connecting orbits of iterated maps and ODEs. Yu.A. Kuznetsov (Utrecht University, NL)

Lecture 5. Numerical continuation of connecting orbits of iterated maps and ODEs. Yu.A. Kuznetsov (Utrecht University, NL) Lecture 5 Numerical continuation of connecting orbits of iterated maps and ODEs Yu.A. Kuznetsov (Utrecht University, NL) May 26, 2009 1 Contents 1. Point-to-point connections. 2. Continuation of homoclinic

More information

Dynamical Systems in Neuroscience: The Geometry of Excitability and Bursting

Dynamical Systems in Neuroscience: The Geometry of Excitability and Bursting Dynamical Systems in Neuroscience: The Geometry of Excitability and Bursting Eugene M. Izhikevich The MIT Press Cambridge, Massachusetts London, England Contents Preface xv 1 Introduction 1 1.1 Neurons

More information

8.1 Bifurcations of Equilibria

8.1 Bifurcations of Equilibria 1 81 Bifurcations of Equilibria Bifurcation theory studies qualitative changes in solutions as a parameter varies In general one could study the bifurcation theory of ODEs PDEs integro-differential equations

More information

Mathematical Foundations of Neuroscience - Lecture 7. Bifurcations II.

Mathematical Foundations of Neuroscience - Lecture 7. Bifurcations II. Mathematical Foundations of Neuroscience - Lecture 7. Bifurcations II. Filip Piękniewski Faculty of Mathematics and Computer Science, Nicolaus Copernicus University, Toruń, Poland Winter 2009/2010 Filip

More information

B5.6 Nonlinear Systems

B5.6 Nonlinear Systems B5.6 Nonlinear Systems 5. Global Bifurcations, Homoclinic chaos, Melnikov s method Alain Goriely 2018 Mathematical Institute, University of Oxford Table of contents 1. Motivation 1.1 The problem 1.2 A

More information

Analysis of the Takens-Bogdanov bifurcation on m parameterized vector fields

Analysis of the Takens-Bogdanov bifurcation on m parameterized vector fields Analysis of the Takens-Bogdanov bifurcation on m parameterized vector fields Francisco Armando Carrillo Navarro, Fernando Verduzco G., Joaquín Delgado F. Programa de Doctorado en Ciencias (Matemáticas),

More information

DIFFERENTIAL EQUATIONS, DYNAMICAL SYSTEMS, AND AN INTRODUCTION TO CHAOS

DIFFERENTIAL EQUATIONS, DYNAMICAL SYSTEMS, AND AN INTRODUCTION TO CHAOS DIFFERENTIAL EQUATIONS, DYNAMICAL SYSTEMS, AND AN INTRODUCTION TO CHAOS Morris W. Hirsch University of California, Berkeley Stephen Smale University of California, Berkeley Robert L. Devaney Boston University

More information

DIFFERENTIAL EQUATIONS, DYNAMICAL SYSTEMS, AND AN INTRODUCTION TO CHAOS

DIFFERENTIAL EQUATIONS, DYNAMICAL SYSTEMS, AND AN INTRODUCTION TO CHAOS DIFFERENTIAL EQUATIONS, DYNAMICAL SYSTEMS, AND AN INTRODUCTION TO CHAOS Morris W. Hirsch University of California, Berkeley Stephen Smale University of California, Berkeley Robert L. Devaney Boston University

More information

BIFURCATION PHENOMENA Lecture 1: Qualitative theory of planar ODEs

BIFURCATION PHENOMENA Lecture 1: Qualitative theory of planar ODEs BIFURCATION PHENOMENA Lecture 1: Qualitative theory of planar ODEs Yuri A. Kuznetsov August, 2010 Contents 1. Solutions and orbits. 2. Equilibria. 3. Periodic orbits and limit cycles. 4. Homoclinic orbits.

More information

Homoclinic saddle to saddle-focus transitions in 4D systems

Homoclinic saddle to saddle-focus transitions in 4D systems Faculty of Electrical Engineering, Mathematics & Computer Science Homoclinic saddle to saddle-focus transitions in 4D systems Manu Kalia M.Sc. Thesis July 2017 Assessment committee: Prof. Dr. S. A. van

More information

In these chapter 2A notes write vectors in boldface to reduce the ambiguity of the notation.

In these chapter 2A notes write vectors in boldface to reduce the ambiguity of the notation. 1 2 Linear Systems In these chapter 2A notes write vectors in boldface to reduce the ambiguity of the notation 21 Matrix ODEs Let and is a scalar A linear function satisfies Linear superposition ) Linear

More information

Homoclinic Orbits of Planar Maps: Asymptotics and Mel nikov Functions

Homoclinic Orbits of Planar Maps: Asymptotics and Mel nikov Functions Department of Mathematics Mathematical Sciences Homoclinic Orbits of Planar Maps: Asymptotics and Mel nikov Functions A thesis submitted for the degree of Master of Science Author: Dirk van Kekem Project

More information

On low speed travelling waves of the Kuramoto-Sivashinsky equation.

On low speed travelling waves of the Kuramoto-Sivashinsky equation. On low speed travelling waves of the Kuramoto-Sivashinsky equation. Jeroen S.W. Lamb Joint with Jürgen Knobloch (Ilmenau, Germany) Marco-Antonio Teixeira (Campinas, Brazil) Kevin Webster (Imperial College

More information

Dynamical Systems. Pierre N.V. Tu. An Introduction with Applications in Economics and Biology Second Revised and Enlarged Edition.

Dynamical Systems. Pierre N.V. Tu. An Introduction with Applications in Economics and Biology Second Revised and Enlarged Edition. Pierre N.V. Tu Dynamical Systems An Introduction with Applications in Economics and Biology Second Revised and Enlarged Edition With 105 Figures Springer-Verlag Berlin Heidelberg New York London Paris

More information

10 Back to planar nonlinear systems

10 Back to planar nonlinear systems 10 Back to planar nonlinear sstems 10.1 Near the equilibria Recall that I started talking about the Lotka Volterra model as a motivation to stud sstems of two first order autonomous equations of the form

More information

One Dimensional Dynamical Systems

One Dimensional Dynamical Systems 16 CHAPTER 2 One Dimensional Dynamical Systems We begin by analyzing some dynamical systems with one-dimensional phase spaces, and in particular their bifurcations. All equations in this Chapter are scalar

More information

Problem set 7 Math 207A, Fall 2011 Solutions

Problem set 7 Math 207A, Fall 2011 Solutions Problem set 7 Math 207A, Fall 2011 s 1. Classify the equilibrium (x, y) = (0, 0) of the system x t = x, y t = y + x 2. Is the equilibrium hyperbolic? Find an equation for the trajectories in (x, y)- phase

More information

computer session iv: Two-parameter bifurcation analysis of equilibria and limit cycles with matcont

computer session iv: Two-parameter bifurcation analysis of equilibria and limit cycles with matcont computer session iv: Two-parameter bifurcation analysis of equilibria and limit cycles with matcont Yu.A. Kuznetsov Department of Mathematics Utrecht University Budapestlaan 6 3508 TA, Utrecht May 16,

More information

Introduction to Bifurcation and Normal Form theories

Introduction to Bifurcation and Normal Form theories Introduction to Bifurcation and Normal Form theories Romain Veltz / Olivier Faugeras October 9th 2013 ENS - Master MVA / Paris 6 - Master Maths-Bio (2013-2014) Outline 1 Invariant sets Limit cycles Stable/Unstable

More information

Example of a Blue Sky Catastrophe

Example of a Blue Sky Catastrophe PUB:[SXG.TEMP]TRANS2913EL.PS 16-OCT-2001 11:08:53.21 SXG Page: 99 (1) Amer. Math. Soc. Transl. (2) Vol. 200, 2000 Example of a Blue Sky Catastrophe Nikolaĭ Gavrilov and Andrey Shilnikov To the memory of

More information

Mathematical Modeling I

Mathematical Modeling I Mathematical Modeling I Dr. Zachariah Sinkala Department of Mathematical Sciences Middle Tennessee State University Murfreesboro Tennessee 37132, USA November 5, 2011 1d systems To understand more complex

More information

Application demonstration. BifTools. Maple Package for Bifurcation Analysis in Dynamical Systems

Application demonstration. BifTools. Maple Package for Bifurcation Analysis in Dynamical Systems Application demonstration BifTools Maple Package for Bifurcation Analysis in Dynamical Systems Introduction Milen Borisov, Neli Dimitrova Department of Biomathematics Institute of Mathematics and Informatics

More information

Torus Maps from Weak Coupling of Strong Resonances

Torus Maps from Weak Coupling of Strong Resonances Torus Maps from Weak Coupling of Strong Resonances John Guckenheimer Alexander I. Khibnik October 5, 1999 Abstract This paper investigates a family of diffeomorphisms of the two dimensional torus derived

More information

Lectures on Dynamical Systems. Anatoly Neishtadt

Lectures on Dynamical Systems. Anatoly Neishtadt Lectures on Dynamical Systems Anatoly Neishtadt Lectures for Mathematics Access Grid Instruction and Collaboration (MAGIC) consortium, Loughborough University, 2007 Part 3 LECTURE 14 NORMAL FORMS Resonances

More information

Ordinary Differential Equations and Smooth Dynamical Systems

Ordinary Differential Equations and Smooth Dynamical Systems D.V. Anosov S.Kh. Aranson V.l. Arnold I.U. Bronshtein V.Z. Grines Yu.S. Il'yashenko Ordinary Differential Equations and Smooth Dynamical Systems With 25 Figures Springer I. Ordinary Differential Equations

More information

Bifurcation of Fixed Points

Bifurcation of Fixed Points Bifurcation of Fixed Points CDS140B Lecturer: Wang Sang Koon Winter, 2005 1 Introduction ẏ = g(y, λ). where y R n, λ R p. Suppose it has a fixed point at (y 0, λ 0 ), i.e., g(y 0, λ 0 ) = 0. Two Questions:

More information

Shilnikov bifurcations in the Hopf-zero singularity

Shilnikov bifurcations in the Hopf-zero singularity Shilnikov bifurcations in the Hopf-zero singularity Geometry and Dynamics in interaction Inma Baldomá, Oriol Castejón, Santiago Ibáñez, Tere M-Seara Observatoire de Paris, 15-17 December 2017, Paris Tere

More information

Stability Analysis of Uzawa-Lucas Endogenous Growth Model

Stability Analysis of Uzawa-Lucas Endogenous Growth Model Abstract: Stability Analysis of Uzawa-Lucas Endogenous Growth Model William A. Barnett* University of Kansas, Lawrence and Center for Financial Stability, NY City and Taniya Ghosh Indira Gandhi Institute

More information

Continuation of cycle-to-cycle connections in 3D ODEs

Continuation of cycle-to-cycle connections in 3D ODEs HET p. 1/2 Continuation of cycle-to-cycle connections in 3D ODEs Yuri A. Kuznetsov joint work with E.J. Doedel, B.W. Kooi, and G.A.K. van Voorn HET p. 2/2 Contents Previous works Truncated BVP s with projection

More information

tutorial ii: One-parameter bifurcation analysis of equilibria with matcont

tutorial ii: One-parameter bifurcation analysis of equilibria with matcont tutorial ii: One-parameter bifurcation analysis of equilibria with matcont Yu.A. Kuznetsov Department of Mathematics Utrecht University Budapestlaan 6 3508 TA, Utrecht February 13, 2018 1 This session

More information

The fold-flip bifurcation

The fold-flip bifurcation The fold-flip bifurcation Yu.A. Kuznetsov, H.G.E. Meijer, and L. van Veen March 0, 003 Abstract The fold-flip bifurcation occurs if a map has a fixed point with multipliers + and simultaneously. In this

More information

Blow-up of vector fields and dynamical systems of compactified Painleve equations

Blow-up of vector fields and dynamical systems of compactified Painleve equations Blow-up of vector fields and dynamical systems of compactified Painleve equations Institute of Mathematics for Industry Kyushu University Hayato Chiba chiba@imi.kyushu-u.ac.jp Nov/29/2012 Introduction

More information

The Transition to Chaos

The Transition to Chaos Linda E. Reichl The Transition to Chaos Conservative Classical Systems and Quantum Manifestations Second Edition With 180 Illustrations v I.,,-,,t,...,* ', Springer Dedication Acknowledgements v vii 1

More information

BIFURCATIONS AND CHAOS IN A PERIODICALLY FORCED PROTOTYPE ADAPTIVE CONTROL SYSTEM 1

BIFURCATIONS AND CHAOS IN A PERIODICALLY FORCED PROTOTYPE ADAPTIVE CONTROL SYSTEM 1 KYBERNETIKA VOLUME 3 0 (1994), NUMBER 2, PAG ES 121-128 BIFURCATIONS AND CHAOS IN A PERIODICALLY FORCED PROTOTYPE ADAPTIVE CONTROL SYSTEM 1 YURI A. KUZNETSOV AND CARLO PICCARDI An adaptive control system

More information

Towards a Global Theory of Singularly Perturbed Dynamical Systems John Guckenheimer Cornell University

Towards a Global Theory of Singularly Perturbed Dynamical Systems John Guckenheimer Cornell University Towards a Global Theory of Singularly Perturbed Dynamical Systems John Guckenheimer Cornell University Dynamical systems with multiple time scales arise naturally in many domains. Models of neural systems

More information

DYNAMICAL SYSTEMS WITH A CODIMENSION-ONE INVARIANT MANIFOLD: THE UNFOLDINGS AND ITS BIFURCATIONS

DYNAMICAL SYSTEMS WITH A CODIMENSION-ONE INVARIANT MANIFOLD: THE UNFOLDINGS AND ITS BIFURCATIONS International Journal of Bifurcation and Chaos c World Scientific Publishing Company DYNAMICAL SYSTEMS WITH A CODIMENSION-ONE INVARIANT MANIFOLD: THE UNFOLDINGS AND ITS BIFURCATIONS KIE VAN IVANKY SAPUTRA

More information

CENTER MANIFOLD AND NORMAL FORM THEORIES

CENTER MANIFOLD AND NORMAL FORM THEORIES 3 rd Sperlonga Summer School on Mechanics and Engineering Sciences 3-7 September 013 SPERLONGA CENTER MANIFOLD AND NORMAL FORM THEORIES ANGELO LUONGO 1 THE CENTER MANIFOLD METHOD Existence of an invariant

More information

2.10 Saddles, Nodes, Foci and Centers

2.10 Saddles, Nodes, Foci and Centers 2.10 Saddles, Nodes, Foci and Centers In Section 1.5, a linear system (1 where x R 2 was said to have a saddle, node, focus or center at the origin if its phase portrait was linearly equivalent to one

More information

7 Planar systems of linear ODE

7 Planar systems of linear ODE 7 Planar systems of linear ODE Here I restrict my attention to a very special class of autonomous ODE: linear ODE with constant coefficients This is arguably the only class of ODE for which explicit solution

More information

APPLIED SYMBOLIC DYNAMICS AND CHAOS

APPLIED SYMBOLIC DYNAMICS AND CHAOS DIRECTIONS IN CHAOS VOL. 7 APPLIED SYMBOLIC DYNAMICS AND CHAOS Bai-Lin Hao Wei-Mou Zheng The Institute of Theoretical Physics Academia Sinica, China Vfö World Scientific wl Singapore Sinaaoore NewJersev

More information

Alligood, K. T., Sauer, T. D. & Yorke, J. A. [1997], Chaos: An Introduction to Dynamical Systems, Springer-Verlag, New York.

Alligood, K. T., Sauer, T. D. & Yorke, J. A. [1997], Chaos: An Introduction to Dynamical Systems, Springer-Verlag, New York. Bibliography Alligood, K. T., Sauer, T. D. & Yorke, J. A. [1997], Chaos: An Introduction to Dynamical Systems, Springer-Verlag, New York. Amann, H. [1990], Ordinary Differential Equations: An Introduction

More information

Nonlinear Autonomous Dynamical systems of two dimensions. Part A

Nonlinear Autonomous Dynamical systems of two dimensions. Part A Nonlinear Autonomous Dynamical systems of two dimensions Part A Nonlinear Autonomous Dynamical systems of two dimensions x f ( x, y), x(0) x vector field y g( xy, ), y(0) y F ( f, g) 0 0 f, g are continuous

More information

Bifurcation Analysis of Neuronal Bursters Models

Bifurcation Analysis of Neuronal Bursters Models Bifurcation Analysis of Neuronal Bursters Models B. Knowlton, W. McClure, N. Vu REU Final Presentation August 3, 2017 Overview Introduction Stability Bifurcations The Hindmarsh-Rose Model Our Contributions

More information

Barcelona, Spain. RTBP, collinear points, periodic orbits, homoclinic orbits. Resumen

Barcelona, Spain.   RTBP, collinear points, periodic orbits, homoclinic orbits. Resumen XX Congreso de Ecuaciones Diferenciales y Aplicaciones X Congreso de Matemática Aplicada Sevilla, 24-28 septiembre 27 (pp. 1 8) The dynamics around the collinear point L 3 of the RTBP E. Barrabés 1, J.M.

More information

2 Qualitative theory of non-smooth dynamical systems

2 Qualitative theory of non-smooth dynamical systems 2 Qualitative theory of non-smooth dynamical systems In this chapter, we give an overview of the basic theory of both smooth and non-smooth dynamical systems, to be expanded upon in later chapters. In

More information

Chapter 23. Predicting Chaos The Shift Map and Symbolic Dynamics

Chapter 23. Predicting Chaos The Shift Map and Symbolic Dynamics Chapter 23 Predicting Chaos We have discussed methods for diagnosing chaos, but what about predicting the existence of chaos in a dynamical system. This is a much harder problem, and it seems that the

More information

Connecting Orbits with Bifurcating End Points

Connecting Orbits with Bifurcating End Points Connecting Orbits with Bifurcating End Points Thorsten Hüls Fakultät für Mathematik Universität Bielefeld Postfach 100131, 33501 Bielefeld Germany huels@mathematik.uni-bielefeld.de June 24, 2004 Abstract

More information

Hopf saddle-node bifurcation for fixed points of 3D-diffeomorphisms: Analysis of a resonance bubble

Hopf saddle-node bifurcation for fixed points of 3D-diffeomorphisms: Analysis of a resonance bubble Physica D www.elsevier.com/locate/physd Hopf saddle-node bifurcation for fixed points of 3D-diffeomorphisms: Analysis of a resonance bubble Henk Broer a, Carles Simó b, Renato Vitolo c, a Department of

More information

Problem set 6 Math 207A, Fall 2011 Solutions. 1. A two-dimensional gradient system has the form

Problem set 6 Math 207A, Fall 2011 Solutions. 1. A two-dimensional gradient system has the form Problem set 6 Math 207A, Fall 2011 s 1 A two-dimensional gradient sstem has the form x t = W (x,, x t = W (x, where W (x, is a given function (a If W is a quadratic function W (x, = 1 2 ax2 + bx + 1 2

More information

Hopf-saddle-node bifurcation for fixed points of 3D-diffeomorphisms: analysis of a resonance bubble

Hopf-saddle-node bifurcation for fixed points of 3D-diffeomorphisms: analysis of a resonance bubble Hopf-saddle-node bifurcation for fixed points of 3D-diffeomorphisms: analysis of a resonance bubble Henk Broer, Carles Simó and Renato Vitolo July 16, 27 Abstract The dynamics near a Hopf-saddle-node bifurcation

More information

APPPHYS217 Tuesday 25 May 2010

APPPHYS217 Tuesday 25 May 2010 APPPHYS7 Tuesday 5 May Our aim today is to take a brief tour of some topics in nonlinear dynamics. Some good references include: [Perko] Lawrence Perko Differential Equations and Dynamical Systems (Springer-Verlag

More information

CHAPTER 6 HOPF-BIFURCATION IN A TWO DIMENSIONAL NONLINEAR DIFFERENTIAL EQUATION

CHAPTER 6 HOPF-BIFURCATION IN A TWO DIMENSIONAL NONLINEAR DIFFERENTIAL EQUATION CHAPTER 6 HOPF-BIFURCATION IN A TWO DIMENSIONAL NONLINEAR DIFFERENTIAL EQUATION [Discussion on this chapter is based on our paper entitled Hopf-Bifurcation Ina Two Dimensional Nonlinear Differential Equation,

More information

The Hopf-van der Pol System: Failure of a Homotopy Method

The Hopf-van der Pol System: Failure of a Homotopy Method DOI.7/s259--9-5 ORIGINAL RESEARCH The Hopf-van der Pol System: Failure of a Homotopy Method H. G. E. Meijer T. Kalmár-Nagy Foundation for Scientific Research and Technological Innovation 2 Abstract The

More information

Dynamics of Modified Leslie-Gower Predator-Prey Model with Predator Harvesting

Dynamics of Modified Leslie-Gower Predator-Prey Model with Predator Harvesting International Journal of Basic & Applied Sciences IJBAS-IJENS Vol:13 No:05 55 Dynamics of Modified Leslie-Gower Predator-Prey Model with Predator Harvesting K. Saleh Department of Mathematics, King Fahd

More information

2 Lecture 2: Amplitude equations and Hopf bifurcations

2 Lecture 2: Amplitude equations and Hopf bifurcations Lecture : Amplitude equations and Hopf bifurcations This lecture completes the brief discussion of steady-state bifurcations by discussing vector fields that describe the dynamics near a bifurcation. From

More information

Hopf bifurcation with zero frequency and imperfect SO(2) symmetry

Hopf bifurcation with zero frequency and imperfect SO(2) symmetry Hopf bifurcation with zero frequency and imperfect SO(2) symmetry F. Marques a,, A. Meseguer a, J. M. Lopez b, J. R. Pacheco b,c a Departament de Física Aplicada, Universitat Politècnica de Catalunya,

More information

Hamiltonian Chaos and the standard map

Hamiltonian Chaos and the standard map Hamiltonian Chaos and the standard map Outline: What happens for small perturbation? Questions of long time stability? Poincare section and twist maps. Area preserving mappings. Standard map as time sections

More information

Weierstraß-Institut. für Angewandte Analysis und Stochastik. Leibniz-Institut im Forschungsverbund Berlin e. V. Preprint ISSN

Weierstraß-Institut. für Angewandte Analysis und Stochastik. Leibniz-Institut im Forschungsverbund Berlin e. V. Preprint ISSN Weierstraß-Institut für Angewandte Analysis und Stochastik Leibniz-Institut im Forschungsverbund Berlin e. V. Preprint ISSN 198-8 Construction of generalized pendulum equations with prescribed maximum

More information

Survey of strong normal-internal k : l resonances in quasi-periodically driven oscillators for l = 1, 2, 3.

Survey of strong normal-internal k : l resonances in quasi-periodically driven oscillators for l = 1, 2, 3. June, : WSPC - Proceedings Trim Size: in x in SPT-broer Survey of strong normal-internal k : l resonances in quasi-periodically driven oscillators for l =,,. H.W. BROER and R. VAN DIJK Institute for mathematics

More information

Course Description - Master in of Mathematics Comprehensive exam& Thesis Tracks

Course Description - Master in of Mathematics Comprehensive exam& Thesis Tracks Course Description - Master in of Mathematics Comprehensive exam& Thesis Tracks 1309701 Theory of ordinary differential equations Review of ODEs, existence and uniqueness of solutions for ODEs, existence

More information

Numerical techniques: Deterministic Dynamical Systems

Numerical techniques: Deterministic Dynamical Systems Numerical techniques: Deterministic Dynamical Systems Henk Dijkstra Institute for Marine and Atmospheric research Utrecht, Department of Physics and Astronomy, Utrecht, The Netherlands Transition behavior

More information

IMPROVED HOMOCLINIC PREDICTOR FOR BOGDANOV-TAKENS BIFURCATION

IMPROVED HOMOCLINIC PREDICTOR FOR BOGDANOV-TAKENS BIFURCATION International Journal of Bifurcation and Chaos c World Scientific Publishing Company IMPROVED HOMOCLINIC PREDICTOR FOR BOGDANOV-TAKENS BIFURCATION YU.A. KUZNETSOV, H.G.E. MEIJER Department of Applied Mathematics,

More information

Defining Equations for Bifurcations and Singularities

Defining Equations for Bifurcations and Singularities Defining Equations for Bifurcations and Singularities John Guckenheimer and Yongjian Xiang Mathematics Department, Ithaca, NY 14853 For Vladimir Arnold on the occasion of his 65th birthday July 1, 2002

More information

Here f and f2 are holomorphic functions of the state variables x; _x; y; _y and parameters 2 R k. These functions are \higher order" in the sense that

Here f and f2 are holomorphic functions of the state variables x; _x; y; _y and parameters 2 R k. These functions are \higher order in the sense that Interactions of Andronov-Hopf and Bogdanov-Takens Bifurcations W. F. Langford and K. Zhan Department of Mathematics and Statistics University of Guelph Guelph, Ontario, Canada NG 2W June 5, 998 Abstract

More information

APPLIED NONLINEAR DYNAMICS

APPLIED NONLINEAR DYNAMICS APPLIED NONLINEAR DYNAMICS Analytical, Computational, and Experimental Methods Ali H. Nayfeh Virginia Polytechnic Institute and State University Balakumar Balachandran University of Maryland WILEY- VCH

More information

Elsevier Editorial System(tm) for Physica D: Nonlinear Phenomena Manuscript Draft

Elsevier Editorial System(tm) for Physica D: Nonlinear Phenomena Manuscript Draft Elsevier Editorial System(tm) for Physica D: Nonlinear Phenomena Manuscript Draft Manuscript Number: Title: Hopf bifurcation with zero frequency and imperfect SO(2) symmetry Article Type: Full Length Article

More information

Hopf bifurcation in coupled cell networks with abelian symmetry 1

Hopf bifurcation in coupled cell networks with abelian symmetry 1 Hopf bifurcation in coupled cell networks with abelian symmetry 1 Ana Paula S. Dias e Rui C. Paiva CMUP Departamento de Matemática Universidade do Porto CMUP Instituto Politécnico de Leiria Abstract We

More information

HOPF BIFURCATION AND HETEROCLINIC CYCLES IN A CLASS OF D 2 EQUIVARIANT SYSTEMS

HOPF BIFURCATION AND HETEROCLINIC CYCLES IN A CLASS OF D 2 EQUIVARIANT SYSTEMS HOPF BIFURCATION AND HETEROCLINIC CYCLES IN A CLASS OF D 2 EQUIVARIANT SYSTEMS ADRIAN C. MURZA Communicated by Vasile Brînzănescu In this paper, we analyze a generic dynamical system with D 2 constructed

More information

An Undergraduate s Guide to the Hartman-Grobman and Poincaré-Bendixon Theorems

An Undergraduate s Guide to the Hartman-Grobman and Poincaré-Bendixon Theorems An Undergraduate s Guide to the Hartman-Grobman and Poincaré-Bendixon Theorems Scott Zimmerman MATH181HM: Dynamical Systems Spring 2008 1 Introduction The Hartman-Grobman and Poincaré-Bendixon Theorems

More information

Examples include: (a) the Lorenz system for climate and weather modeling (b) the Hodgkin-Huxley system for neuron modeling

Examples include: (a) the Lorenz system for climate and weather modeling (b) the Hodgkin-Huxley system for neuron modeling 1 Introduction Many natural processes can be viewed as dynamical systems, where the system is represented by a set of state variables and its evolution governed by a set of differential equations. Examples

More information

27. Topological classification of complex linear foliations

27. Topological classification of complex linear foliations 27. Topological classification of complex linear foliations 545 H. Find the expression of the corresponding element [Γ ε ] H 1 (L ε, Z) through [Γ 1 ε], [Γ 2 ε], [δ ε ]. Problem 26.24. Prove that for any

More information

Numerical Continuation of Bifurcations - An Introduction, Part I

Numerical Continuation of Bifurcations - An Introduction, Part I Numerical Continuation of Bifurcations - An Introduction, Part I given at the London Dynamical Systems Group Graduate School 2005 Thomas Wagenknecht, Jan Sieber Bristol Centre for Applied Nonlinear Mathematics

More information

Small aspect ratio Taylor-Couette flow: Onset of a very-low-frequency three-torus state

Small aspect ratio Taylor-Couette flow: Onset of a very-low-frequency three-torus state PHYSICAL REVIEW E 68, 036302 2003 Small aspect ratio Taylor-Couette flow: Onset of a very-low-frequency three-torus state Juan M. Lopez* Department of Mathematics and Statistics, Arizona State University,

More information

Continuous Threshold Policy Harvesting in Predator-Prey Models

Continuous Threshold Policy Harvesting in Predator-Prey Models Continuous Threshold Policy Harvesting in Predator-Prey Models Jon Bohn and Kaitlin Speer Department of Mathematics, University of Wisconsin - Madison Department of Mathematics, Baylor University July

More information

Dynamical Systems in Neuroscience: Elementary Bifurcations

Dynamical Systems in Neuroscience: Elementary Bifurcations Dynamical Systems in Neuroscience: Elementary Bifurcations Foris Kuang May 2017 1 Contents 1 Introduction 3 2 Definitions 3 3 Hodgkin-Huxley Model 3 4 Morris-Lecar Model 4 5 Stability 5 5.1 Linear ODE..............................................

More information

( Bx + f(x, y) Cy + g(x, y)

( Bx + f(x, y) Cy + g(x, y) Chapter 6 Center manifold reduction The previous chaper gave a rather detailed description of bifurcations of equilibria and fixed points in generic one-parameter families of ODEs and maps with minimal

More information

In Arnold s Mathematical Methods of Classical Mechanics (1), it

In Arnold s Mathematical Methods of Classical Mechanics (1), it Near strongly resonant periodic orbits in a Hamiltonian system Vassili Gelfreich* Mathematics Institute, University of Warwick, Coventry CV4 7AL, United Kingdom Communicated by John N. Mather, Princeton

More information

B5.6 Nonlinear Systems

B5.6 Nonlinear Systems B5.6 Nonlinear Systems 4. Bifurcations Alain Goriely 2018 Mathematical Institute, University of Oxford Table of contents 1. Local bifurcations for vector fields 1.1 The problem 1.2 The extended centre

More information

Interactions of Andronov{Hopf. and Bogdanov{Takens Bifurcations. Abstract. A codimension-three bifurcation, characterized by a pair of purely

Interactions of Andronov{Hopf. and Bogdanov{Takens Bifurcations. Abstract. A codimension-three bifurcation, characterized by a pair of purely Interactions of Andronov{Hopf and Bogdanov{Takens Bifurcations William F. Langford and Kaijun Zhan Abstract. A codimension-three bifurcation, characterized by a pair of purely imaginary eigenvalues and

More information

7 Two-dimensional bifurcations

7 Two-dimensional bifurcations 7 Two-dimensional bifurcations As in one-dimensional systems: fixed points may be created, destroyed, or change stability as parameters are varied (change of topological equivalence ). In addition closed

More information

Local Bifurcations, Center Manifolds, and Normal Forms in Infinite-Dimensional Dynamical Systems

Local Bifurcations, Center Manifolds, and Normal Forms in Infinite-Dimensional Dynamical Systems Local Bifurcations, Center Manifolds, and Normal Forms in Infinite-Dimensional Dynamical Systems Universitext For other titles published in this series, go to www.springer.com/series/223 Mariana Haragus

More information

Identification of one-parameter bifurcations giving rise to periodic orbits, from their period function

Identification of one-parameter bifurcations giving rise to periodic orbits, from their period function Identification of one-parameter bifurcations giving rise to periodic orbits, from their period function Armengol Gasull 1, Víctor Mañosa 2, and Jordi Villadelprat 3 1 Departament de Matemàtiques Universitat

More information

THE CUSP HOPF BIFURCATION *

THE CUSP HOPF BIFURCATION * International Journal of Bifurcation and Chaos, Vol. 17, No. 8 (2007) 2547 2570 c World Scientific Publishing Company THE CUSP HOPF BIFURCATION * J. HARLIM Courant Institute of Mathematical Sciences, New

More information

Computational Methods in Dynamical Systems and Advanced Examples

Computational Methods in Dynamical Systems and Advanced Examples and Advanced Examples Obverse and reverse of the same coin [head and tails] Jorge Galán Vioque and Emilio Freire Macías Universidad de Sevilla July 2015 Outline Lecture 1. Simulation vs Continuation. How

More information

Differential Equations and Dynamical Systems

Differential Equations and Dynamical Systems Differential Equations and Dynamical Systems Péter L. Simon Eötvös Loránd University Institute of Mathematics Department of Applied Analysis and Computational Mathematics 2012 Contents 1 Introduction 2

More information

Introduction to Continuous Dynamical Systems

Introduction to Continuous Dynamical Systems Lecture Notes on Introduction to Continuous Dynamical Systems Fall, 2012 Lee, Keonhee Department of Mathematics Chungnam National Univeristy - 1 - Chap 0. Introduction What is a dynamical system? A dynamical

More information

On dynamical properties of multidimensional diffeomorphisms from Newhouse regions: I

On dynamical properties of multidimensional diffeomorphisms from Newhouse regions: I IOP PUBLISHING Nonlinearity 2 (28) 923 972 NONLINEARITY doi:.88/95-775/2/5/3 On dynamical properties of multidimensional diffeomorphisms from Newhouse regions: I S V Gonchenko, L P Shilnikov and D V Turaev

More information

Homoclinic and heteroclinic bifurcations close to a twisted. heteroclinic cycle. Martn G. Zimmermann, Dept. of Quantum Chemistry. Uppsala University

Homoclinic and heteroclinic bifurcations close to a twisted. heteroclinic cycle. Martn G. Zimmermann, Dept. of Quantum Chemistry. Uppsala University Homoclinic and heteroclinic bifurcations close to a twisted heteroclinic cycle. Martn G. Zimmermann, Dept. of Quantum Chemistry Uppsala University Box 58, S-75 UPPSALA, Sweden and Mario A. Natiello y Dept.

More information

Vector Field Topology. Ronald Peikert SciVis Vector Field Topology 8-1

Vector Field Topology. Ronald Peikert SciVis Vector Field Topology 8-1 Vector Field Topology Ronald Peikert SciVis 2007 - Vector Field Topology 8-1 Vector fields as ODEs What are conditions for existence and uniqueness of streamlines? For the initial value problem i x ( t)

More information

Bifurcations In Reversible Systems With Application To The Michelson System

Bifurcations In Reversible Systems With Application To The Michelson System Bifurcations In Reversible Systems With Application To The Michelson System A thesis presented for the degree of Doctor of Philosophy of the University of London and the Diploma of Membership for Imperial

More information

Bifurcations of maps: numerical algorithms and applications

Bifurcations of maps: numerical algorithms and applications main 2008/2/28 17:19 page i #1 Bifurcations of maps: numerical algorithms and applications Reza Khoshsiar Ghaziani 1 0.5 0 0.5 1 1.5 2 2.5 2 1.5 1 0.5 0 0.5 1 Supervisor: Prof. Dr. W. Govaerts Co-supervisor:

More information

On the Takens-Bogdanov Bifurcation in the Chua s Equation

On the Takens-Bogdanov Bifurcation in the Chua s Equation 1722 PAPER Special Section on Nonlinear Theory and Its Applications On the Takens-Bogdanov Bifurcation in the Chua s Equation Antonio ALGABA, Emilio FREIRE, Estanislao GAMERO, and Alejandro J. RODRÍGUEZ-LUIS,

More information

1. (i) Determine how many periodic orbits and equilibria can be born at the bifurcations of the zero equilibrium of the following system:

1. (i) Determine how many periodic orbits and equilibria can be born at the bifurcations of the zero equilibrium of the following system: 1. (i) Determine how many periodic orbits and equilibria can be born at the bifurcations of the zero equilibrium of the following system: ẋ = y x 2, ẏ = z + xy, ż = y z + x 2 xy + y 2 + z 2 x 4. (ii) Determine

More information

8 Vector Field Topology

8 Vector Field Topology Vector fields as ODEs What are conditions for eistence and uniqueness of streamlines? 8 Vector Field Topology For the initial value problem ( t) = v( ( t) ) i t = 0 0 a solution eists if the velocity field

More information