Nonlinear Dynamics and Chaos
Nonlinear Dynamics and Chaos
2nd Edition
ISBN: 9780813349107
Author: Steven H. Strogatz
Publisher: PERSEUS D
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Chapter 9.6, Problem 5E
Interpretation Introduction

Interpretation:

Consider the receiver dynamics, x˙r=σ(yrxr), y˙r=rs(t)yrs(t)zr and z˙r=s(t)yrbzr. If the receiverhas synchronized with the drive signal, then xr(t)  x(t) , and so, m(t) may be recovered as m^(t)=s(t)xr(t). Test this approachnumericallyusing a sine wave for m(t). Estimate how close m^(t) is to the actual message m(t). Explain how the error depends upon the frequency of the sine wave.

Concept Introduction:

  • ➢ UseLorenz equations by substituting s(t)=x(t)+ m(t)

  • ➢ At the receiver end, the error is a function of m(t).

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