Nonlinear Dynamics and Chaos
Nonlinear Dynamics and Chaos
2nd Edition
ISBN: 9780429972195
Author: Steven H. Strogatz
Publisher: Taylor & Francis
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Chapter 9.1, Problem 3E
Interpretation Introduction

Interpretation:

To find the change of the variables that convert the waterwheel equations to the Lorenz equations.

To show that when waterwheel equations are translated into the Lorenz equations, the Lorenz parameter b becomes b = 1.

Concept Introduction:

  • ➢ The fixed point of a differential equation is a point where f(x*) = 0 ; while substitution f(x*) = x˙ is used and x&*#x00A0;is a fixed point.

  • ➢ The Lorenz system is the system of the ordinary differential equations which have a chaotic solution for the particular parameter values and initial conditions.

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