Nonlinear Dynamics and Chaos
Nonlinear Dynamics and Chaos
2nd Edition
ISBN: 9780813349107
Author: Steven H. Strogatz
Publisher: PERSEUS D
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Chapter 8.6, Problem 2E
Interpretation Introduction

Interpretation:

  • (a) To show that the given system has no fixed points, given that ω1,ω2>0   and   K1,K2>0.

  • (b) To find the conserved quantity for the system.

  • (c) To show that the system can be non-dimensionalized to 1=1 + asin(θ21) ,  2=ω + asin(θ12),

    if it is given that, K1= K2.

  • (d) To find the winding number analytically. (winding number = limτθ1(τ)θ2(τ)).

Concept Introduction:

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

  • ➢ The winding number determines the nature of trajectory. In the case of a rational winding number, the trajectory is a trefoil knot, while in the case of an irrational number, there is no closed solution.

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