Bifurcations in piecewise-smooth systems Chris Budd.

Slides:



Advertisements
Similar presentations
Piecewise-smooth dynamical systems: Bouncing, slipping and switching: 1. Introduction Chris Budd.
Advertisements

Oil and it's products are used constantly in everyday life. This project is concerned with the modelling of the torsional waves that occur during the oil.
2. Piecewise-smooth maps Chris Budd. Maps Key idea … The functions or one of their nth derivatives, differ when Discontinuity set Interesting discontinuity.
III: Hybrid systems and the grazing bifurcation Chris Budd.
Ch 6.4: Differential Equations with Discontinuous Forcing Functions
Domain & Range. When the coordinates are listed; determining the Domain ( D ) and Range ( R ) of a function is quite easy…
Hamiltonian Chaos and the standard map Poincare section and twist maps. Area preserving mappings. Standard map as time sections of kicked oscillator (link.
Chattering: a novel route to chaos in cam-follower impacting systems Ricardo Alzate Ph.D. Student University of Naples FEDERICO II, ITALY Prof. Mario di.
Nonlinear dynamics in a cam- follower impacting system Ricardo Alzate Ph.D. Student University of Naples FEDERICO II (SINCRO GROUP)
1 Predator-Prey Oscillations in Space (again) Sandi Merchant D-dudes meeting November 21, 2005.
Cam-follower systems: experiments and simulations by Ricardo Alzate University of Naples – Federico II WP6: Applications.
GRAPHING CUBIC, SQUARE ROOT AND CUBE ROOT FUNCTIONS.
1 Excursions in Modern Mathematics Sixth Edition Peter Tannenbaum.
2. The Universality of Chaos Some common features found in non-linear systems: Sequences of bifurcations (routes to chaos). Feigenbaum numbers. Ref: P.Cvitanovic,”Universality.
Neuronal excitability from a dynamical systems perspective Mike Famulare CSE/NEUBEH 528 Lecture April 14, 2009.
Logistic Map. Discrete Map  A map f is defined on a metric space X.  Repeated application of f forms a sequence. Discrete set of points  A sequence.
Bifurcation and Resonance Sijbo Holtman Overview Dynamical systems Resonance Bifurcation theory Bifurcation and resonance Conclusion.
Introduction to chaotic dynamics
L Berkley Davis Copyright 2009 MER301: Engineering Reliability Lecture 14 1 MER301: Engineering Reliability LECTURE 14: Chapter 7: Design of Engineering.
CHΑΟS and (un-) predictability Simos Ichtiaroglou Section of Astrophysics, Astronomy and Mechanics Physics Department University of Thessaloniki.
COMPLEXITY OF EARTHQUAKES: LEARNING FROM SIMPLE MECHANICAL MODELS Elbanna, Ahmed and Thomas Heaton Civil Engineering.
Order-Tuned and Impact Absorbers for Rotating Flexible Structures.
Name That Graph…. Parent Graphs or Base Graphs Linear Quadratic Absolute Value Square Root Cubic Exponential Math
Analysis of the Rossler system Chiara Mocenni. Considering only the first two equations and ssuming small z The Rossler equations.
Overview of Kernel Methods Prof. Bennett Math Model of Learning and Discovery 2/27/05 Based on Chapter 2 of Shawe-Taylor and Cristianini.
ORDINARY DIFFERENTIAL EQUATION (ODE) LAPLACE TRANSFORM.
1 GEM2505M Frederick H. Willeboordse Taming Chaos.
Renormalization and chaos in the logistic map. Logistic map Many features of non-Hamiltonian chaos can be seen in this simple map (and other similar one.
1 GEM2505M Frederick H. Willeboordse Taming Chaos.
Confessions of an industrial mathematican Chris Budd.
10/2/2015Electronic Chaos Fall Steven Wright and Amanda Baldwin Special Thanks to Mr. Dan Brunski.
Chaotic Dynamical Systems Experimental Approach Frank Wang.
Introduction to Quantum Chaos
Basins of Attraction Dr. David Chan NCSSM TCM Conference February 1, 2002.
Prepared by Mrs. Azduwin Binti Khasri
Deterministic Chaos and the Chao Circuit
Introduction to Chaos Clint Sprott Department of Physics University of Wisconsin - Madison Presented to Physics 311 at University of Wisconsin in Madison,
1 Universal Bicritical Behavior in Unidirectionally Coupled Systems Sang-Yoon Kim Department of Physics Kangwon National University Korea  Low-dimensional.
THE LAPLACE TRANSFORM LEARNING GOALS Definition
Motivation As we’ve seen, chaos in nonlinear oscillator systems, such as the driven damped pendulum discussed last time is very complicated! –The nonlinear.
Lecture #3 What can go wrong? Trajectories of hybrid systems João P. Hespanha University of California at Santa Barbara Hybrid Control and Switched Systems.
Introduction to synchronization: History
Interactive Graphics Lecture 10: Slide 1 Interactive Computer Graphics Lecture 10 Introduction to Surface Construction.
2D Henon Map The 2D Henon Map is similar to a real model of the forced nonlinear oscillator. The Purpose is The Investigation of The Period Doubling Transition.
Analysis of the Rossler system Chiara Mocenni. Considering only the first two equations and assuming small z, we have: The Rossler equations.
Controlling Chaos Journal presentation by Vaibhav Madhok.
Discrete Dynamic Systems. What is a Dynamical System?
Application of Bifurcation Theory To Current Mode Controlled (CMC) DC-DC Converters.
ECE-7000: Nonlinear Dynamical Systems 3. Phase Space Methods 3.1 Determinism: Uniqueness in phase space We Assume that the system is linear stochastic.
Global Analysis of Impacting Systems Petri T Piiroinen¹, Joanna Mason², Neil Humphries¹ ¹ National University of Ireland, Galway - Ireland ²University.
Introduction to Chaos Clint Sprott
The Cournot duopoly Kopel Model
Sequences Write down the next 3 terms in each sequence:
Including Complex Dynamics in Complex Analysis Courses
Handout #21 Nonlinear Systems and Chaos Most important concepts
Introduction to chaotic dynamics
Strange Attractors From Art to Science
Introduction of Chaos in Electric Drive Systems
Parent Functions.
Qiudong Wang, University of Arizona (Joint With Kening Lu, BYU)
Introduction to chaotic dynamics
Parent Functions.
“An Omnivore Brings Chaos”
Chattering and grazing in impact oscillators
Continuity.
Signals and Systems Lecture 2
Nonlinear oscillators and chaos
Poincare Maps and Hoft Bifurcations
THE LAPLACE TRANSFORM LEARNING GOALS Definition
Finding the Popular Frequency!
Presentation transcript:

Bifurcations in piecewise-smooth systems Chris Budd

What is a piecewise-smooth system? Map Flow Hybrid Heartbeats or Poincare maps Rocking block, friction, Chua circuit Impact or control systems

PWS Flow PWS Sliding Flow Hybrid

Key idea … The functions or one of their nth derivatives, differ when Discontinuity set Interesting discontinuity induced bifurcations occur when limit sets of the flow/map intersect the discontinuity set

Why are we interested in them? Lots of important physical systems are piecewise-smooth: bouncing balls, Newtons cradle, friction, rattle, switching, control systems, DC-DC converters, gear boxes … Piecewise-smooth systems have behaviour which is quite different from smooth systems and is induced by the discontinuity: period adding Much of this behaviour can be analysed, and new forms of discontinuity induced bifurcations can be studied: border collisions, grazing bifurcations, corner collisions.

Will illustrate the behaviour of piecewise smooth systems by looking at Maps Hybrid impacting systems

Some piecewise-smooth maps Linear, discontinuous Square-root, continuous

Both maps have fixed points over certain ranges of Border collision bifurcations occur when for certain parameter values the fixed points intersect with the discontinuity set Get exotic dynamics close to these parameter values

Dynamics of the piecewise-linear map Period adding Farey sequence Fixed point Homoclinic orbit Fixed point

Dynamics of the piecewise-linear map Period adding Farey sequence Chaotic

Square-root map Map arises in the study of grazing bifurcations of flows and hybrid systems Infinite stretching when Fixed point at

Chaos Period adding

Immediate jump to robust chaos Partial period adding

Get similar behaviour in higher-dimensional square-root maps Map [Nordmark] also arises naturally in the study of grazing in flows and hybrid systems.

If A has complex eigenvalues we see discontinuous transitions between periodic orbits If A has real eigenvalues we see similar behaviour to the 1D map

Impact oscillators: a canonical hybrid system obstacle

Periodic dynamics Chaotic dynamics Experimental Analytic

Complex domains of attraction of periodic orbits

Regular and discontinuity induced bifurcations as parameters vary Regular and discontinuity induced bifurcations as parameters vary. Period doubling Grazing

Grazing occurs when periodic orbits intersect the obstacle tanjentially

Observe grazing bifurcations identical to the dynamics of the two-dimensional square-root map Period-adding Transition to a periodic orbit Non-impacting orbit

Local analysis of a Poincare map associated with a grazing periodic orbit shows that this map has a locally square-root form, hence the observed period-adding and similar behaviour Poincare map associated with a grazing periodic orbit of a piecewise-smooth flow typically is smoother (eg. Locally order 3/2 or higher) giving more regular behaviour

Systems of impacting oscillators can have even more exotic behaviour which arises when there are multiple collisions. This can be described by looking at the behaviour of the discontinuous maps

CONCLUSIONS Piecewise-smooth systems have interesting dynamics Some (but not all) of this dynamics can be understood and analysed Many applications and much still to be discovered

Parameter range for simple periodic orbits Fractions 1/nFractions (n-1)/n