Nonlinear Dynamics and Chaos
Nonlinear Dynamics and Chaos
2nd Edition
ISBN: 9780813349107
Author: Steven H. Strogatz
Publisher: PERSEUS D
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Chapter 7.6, Problem 19E
Interpretation Introduction

Interpretation:

For a time τ = ωt, show that the equation transformsinto the ω2x"+x+ε(x)3=0. Also show that O(1):x0"+x0= 0, O(ε):x1"+ x1= - 2ω1x0"- x03, and the initial condition becomes xk(0)= a, xk'(0)=0 for all k > 0. Solve O(1) for x0. Show that after substitution of x0, the O(ε) equation becomes x1"+ x1=(1a- 34a3)cos τ- 14a3cos(). Also solve it for x1.

Concept Introduction:

The system equation for the linear oscillator is x¨  + x = 0. If the system is perturbed by small perturbation constant, the system equation becomes x¨ + x + εh(x,x˙)= 0

Here, 0<ε1 and h(x,x˙) is a smooth function.

This system is known as a weakly nonlinear oscillator.

The expression of the amplitude of any limit cycle for the original system is r = r0+ O(ε)

The expression of the frequency of any limit cycle for the original system is ω = 1+ε ϕ'

Taylor series expansion of x(t,ε) is x(t,ε) - x(t,T) + O(ε). Here, O(ε) are the higher-order terms of the Taylor series expansion.

Taylor’s series expansion (1x)1 is (1- x)-1=1+x+x2+x4+......

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