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Simple Chaotic Systems and Circuits

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Jerk equations for these systems are not very 'simple' Some of the systems found by Sprott have 'simple' jerk forms: Sprott (1997) dx/dt = y ... – PowerPoint PPT presentation

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Title: Simple Chaotic Systems and Circuits


1
Simple Chaotic Systems and Circuits
  • J. C. Sprott
  • Department of Physics
  • University of Wisconsin - Madison
  • Presented at the
  • Gordon Conference on Classical Mechanics and
    Nonlinear Dynamics
  • on June 16, 2004

2
Lorenz Equations (1963)
  • dx/dt Ay Ax
  • dy/dt xz Bx y
  • dz/dt xy Cz
  • 7 terms, 2 quadratic nonlinearities, 3 parameters

3
Rössler Equations (1976)
  • dx/dt y z
  • dy/dt x Ay
  • dz/dt B xz Cz
  • 7 terms, 1 quadratic nonlinearity, 3 parameters

4
Lorenz Quote (1993)
  • One other study left me with mixed feelings.
    Otto Roessler of the University of Tübingen had
    formulated a system of three differential
    equations as a model of a chemical reaction. By
    this time a number of systems of differential
    equations with chaotic solutions had been
    discovered, but I felt I still had the
    distinction of having found the simplest.
    Roessler changed things by coming along with an
    even simpler one. His record still stands.

5
Rössler Toroidal Model (1979)
Probably the simplest strange attractor of a 3-D
ODE
(1998)
  • dx/dt y z
  • dy/dt x
  • dz/dt Ay Ay2 Bz
  • 6 terms, 1 quadratic nonlinearity, 2 parameters

6
Sprott (1994)
  • 14 examples with 6 terms and 1 quadratic
    nonlinearity
  • 5 examples with 5 terms and 2 quadratic
    nonlinearities

J. C. Sprott, Phys. Rev. E 50, R647 (1994)
7
Gottlieb (1996)
  • What is the simplest jerk function that gives
    chaos?
  • Displacement x
  • Velocity dx/dt
  • Acceleration d2x/dt2
  • Jerk d3x/dt3

8
Linz (1997)
  • Lorenz and Rössler systems can be written in jerk
    form
  • Jerk equations for these systems are not very
    simple
  • Some of the systems found by Sprott have simple
    jerk forms

9
Sprott (1997)
Simplest Dissipative Chaotic Flow
  • dx/dt y
  • dy/dt z
  • dz/dt az y2 x
  • 5 terms, 1 quadratic nonlinearity, 1 parameter

10
Bifurcation Diagram
11
Return Map
12
Zhang and Heidel (1997)
  • 3-D quadratic systems with fewer than 5 terms
    cannot be chaotic.
  • They would have no adjustable parameters.

13
Linz and Sprott (1999)
  • dx/dt y
  • dy/dt z
  • dz/dt az y x 1
  • 6 terms, 1 abs nonlinearity, 2 parameters (but
    one 1)

14
General Form
  • dx/dt y
  • dy/dt z
  • dz/dt az y G(x)
  • G(x) (bx c)
  • G(x) b(x2/c c)
  • G(x) b max(x,0) c
  • G(x) (bx c sgn(x))
  • etc.

15
Universal Chaos Approximator?
16
First Circuit
17
Bifurcation Diagram for First Circuit
18
Strange Attractor for First Circuit
Calculated
Measured
19
Second Circuit
20
Chaos Circuit
21
Third Circuit
22
Fourth Circuit
D(x) min(x, 0)
23
Bifurcation Diagram for Fourth Circuit
K. Kiers, D. Schmidt, and J. C. Sprott, Am. J.
Phys. 72, 503 (2004)
24
(No Transcript)
25
References
  • http//sprott.physics.wisc.edu/
    lectures/gordon04.ppt (this talk)
  • http//www.css.tayloru.edu/dsimons/ (circuit 4)
  • sprott_at_physics.wisc.edu (to contact me)
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