Chua s Circuit: The Paradigm for Generating Chaotic Attractors

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Chua s Circuit: The Paradigm for Generating Chaotic Attractors EE129 Fall 2007 Bharathwaj Muthuswamy NOEL: Nonlinear Electronics Lab 151M Cory Hall Department of EECS University of California, Berkeley mbharat@eecs.berkeley.edu http://nonlinear.eecs.berkeley.edu August 30 th 2007

Outline Introduction to Chaos What is Chaos? Chaos in Nature Hallmarks of Chaos Non-periodic behavior in time domain Sensitive dependence on initial conditions Proving the existence of Chaos Easy Chaos: Chua s circuit Building and working with Chua s circuit References Simulating Chua s circuit: MultiSim Turning your PC into an oscilloscope: Osqoop Chua s circuit for high school students Interesting MATLAB experiments Questions

Introduction to Chaos: What is Chaos? There is NO universal agreed-upon definition of Chaos Loosely speaking, a Chaotic system is a deterministic system that exhibits random behavior. Example - Chua s circuit: Set of ordinary differential equations with a simple nonlinearity BUT the system behavior is complex: Time domain Phase space

Chaos in Nature Weather (Reference: Deterministic Nonperiodic Flow. Lorenz, Edward N. Journal of Atmospheric Sciences. pp. 130 141, 1963) A plot of the Lorenz attractor for r = 28, σ = 10, b = 8/3 (Reference: Chaos Theory, Wikipedia Entry. Online at: http://en.wikipedia.org/wiki/chaos_theory)

Chaos in Nature Trajectory of planetary orbits: (Reference: The role of chaotic resonances in the Solar System. Murray, N. and Holman M. Nature. pp. 773 780, vol. 410, 12 April 2001) Irregulary shaped satellites like Hyperion (moon of Saturn) tumble chaotically. Chaos in the orbits of giant planets (Jupiter, Saturn and Uranus) the location of these planets cannot be predicted on a time scale longer than a few tens of millions of years. Quote from the paper above: The worried reader may find some comfort in that the accompanying analytic theory predicts that no planet will be ejected before the Sun dies.

Chaos in Nature Brain waves (Reference: Rhythms of the Brain. Buzsaki, Gyorgy. Oxford University Press. 2006)

Hallmarks of Chaos Non-periodic behavior in the time domain Time series data from neural nodes implanted in rat cortex Reference: Taming Chaos: Stabilization of Aperiodic Attractors by Noise. Freeman, W. et. al. IEEE Trans. On Circuits and Systems I: Fundamental Theory and Applications. Vol. 44, No. 10, Oct. 1997

Hallmarks of Chaos Sensitive dependence on initial conditions Eventually, the paths diverge (mathematically quantified by the Lyapunov exponent) Three initial conditions x 10, x 20 and x 30 (they are arbitrarily close to each other) Reference: http://www.keldysh.ru/departments/dpt_17/eng/ndeng.html

Proving the existence of Chaos Mathematically very challenging: Lorenz s system was proved to be chaotic nearly 40 YEARS after Lorenz s observations: The Lorenz Attractor Exists. Tucker, Warwick. Ph.D. Thesis, 1998. University of Uppsala. One way to prove chaotic behavior: define a homeomorphism to the Cantor set using a Smale horseshoe

Proving the existence of Chaos But for the purposes of EE129: Central concept: Poincare-Bendixson Theorem In a nutshell, the consequence of the theorem is that a continuous time autonomous dynamical system CANNOT be chaotic in the plane (2-dimensions).

Easy Chaos: Chua s circuit Designed using systematic nonlinear circuit techniques by Leon O. Chua in 1983 Excellent Reference: The Genesis of Chua s circuit. Chua, Leon O. Archiv fur Elektronik und Uebertragungstechnik, July 1992, vol. 46, (no. 4): 250-257.

Easy Chaos: Chua s circuit A consequence of the Poincare-Bendixson theorem - we need three independent energy storage elements. Hence:

Easy Chaos: Chua s circuit Nonlinearity designed by Leon so that a proof of Chaos is easy. For details, please refer to The Genesis of Chua s Circuit paper. KEY: We need at least two unstable equilibrium points one to provide stretching dynamics and the other to provide folding.

Easy Chaos: Chua s circuit Existence of these equilibrium points can be seen from DC load line: DC Load line Reference: Three Steps to Chaos Part II: A Chua s Circuit Primer. Kennedy, Michael P. IEEE Trans. On Circuits and Systems I: Fundamental Theory and Applications. Vol. 40, No. 10, Oct. 1993 We will see how we can obtain this nonlinearity later using op-amps

Easy Chaos: Chua s circuit Some properties of Chua s circuit: Chua s circuit is the simplest possible electronic circuit that can exhibit chaotic behavior. Reference: The double scroll family, Parts I and II. Chua et. al. IEEE Trans. On Circuits and Systems. Vol. CAS-33, no. 11, pp. 1073-1118, 1986. Applications of Chua s circuit: Music: Reading Complexity in Chua s Oscillator through Music. Part I: A New Way of Understanding Chaos. Bilotta, Eleonara et. al. International Journal of Bifurcation and Chaos. Vol. 15, No. 2, pp. 253 282. 2005. Communications: Chaotic Digital Encoding: An Approach to Secure Communication. Frey, D.R. IEEE Trans. On Circuits and Systems II: Analog and Digital Signal Processing. Vol. 40, #10, pp. 660 666. Oct. 1993.

Building and working with Chua s circuit Now, we will see how easy it is to build Chua s circuit with readily available components! References NOEL Chaos in Chua s Circuit homepage http://nonlinear.eecs.berkeley.edu/chaos/chaos.html Chaos Wiki: http://robotlab.itk.ppke.hu/~wiki/mediawiki- 1.9.3/index.php/Main_Page Chua s Circuit for High School Students. Gandhi, Gaurav., Muthuswamy, Bharathwaj and Roska, Tamas. To appear in the International Journal of Bifurcation and Chaos in Dec. 2007 preprint copy online Also read (available online): The Genesis of Chua s Circuit Three Steps to Chaos. Part 2 Chua s Circuit Primer

Building and working with Chua s circuit Lecture demo - Simulating Chua s circuit: MultiSim

Building and working with Chua s circuit Lecture Demo - Turning your PC into an oscilloscope: osqoop

Building and working with Chua s circuit Lecture Demo - Chua s circuit for high school students

Building and working with Chua s circuit Chua s circuit for high school students. Debugging Tips: Checking the functionality of the nonlinear resistor Tuning the circuit

Building and working with Chua s circuit Lecture Demo - Interesting MATLAB experiments using Chua s circuit: Sample data from sound card Compute Fourier Transform Compute Autocorrelation coefficient. Compare this to autocorrelation coefficient of white noise.

Questions Reference: http://mathstat.helsinki.fi/mathphys/paolo_files/lorenz11.gif