Nonlinear Dynamics and Chaos
Nonlinear Dynamics and Chaos
2nd Edition
ISBN: 9780813349107
Author: Steven H. Strogatz
Publisher: PERSEUS D
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Chapter 8.4, Problem 11E
Interpretation Introduction

Interpretation:

  • By fixing parameters k =1, b =43, F = 2 and by using the numerical integration plot, the phase portrait for the averaged system, by varying parameter 'a' from negative to positive.

  • To show for a = 2.8 there are two stable points.

  • Numerically integrate the original forced Duffing equation and plot x(t) for 'a' increasing slowly from a = -1 to a = 5 and decreases slowly back to a = -1

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 smooth function.

    This system is known as weakly nonlinear oscillator.

  • The polar transformation of Cartesian co-ordinates is

    x = rcosθy = rsinθ

  • The averaged equations for r and rϕ are

    r=10h(θ)sinθdθh sinθ

    rϕ=10h(θ)cosθdθh cosθ

    Where, h(θ)=h(x,x˙)=h(r cosθ,r sinθ)

  • The value of r0 is calculated as

    r0=(x(0))2+(x˙(0))2

    The value of ϕ0 is calculated by

    ϕ0=tan(x˙(0)x(0))

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