Nonlinear Dynamics and Chaos
Nonlinear Dynamics and Chaos
2nd Edition
ISBN: 9780813349107
Author: Steven H. Strogatz
Publisher: PERSEUS D
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Chapter 12.4, Problem 4E
Interpretation Introduction

Interpretation:

Numerically integrate the Lorenz equations for standard parameters r = 28, b =83, σ =10 and obtain the long time series for x(t) and then by using attractor reconstruction method for various values of the delay and plot (x(t), x(t + τ)) also find the value of τ for which the reconstructed attractor is similar to actual Lorenz attractor.

Concept Introduction:

  • The Lorenz equations are

    x˙=σ(yx)y˙=rxyxzz˙=xybzHere σ, r, b > 0

    The solution of Lorenz equations oscillates irregularly for wide range of parameters, never exactly repeating but always remains in bounded region of phase space.

  • Rössler system is

    x˙=yzy˙=x+ayz˙=b+z(xc)

  • In attractor reconstruction method the time delay τ is introduced, and by observing graphs, for which value of τ the phase space look similar to actual Lorenz attractor.

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