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 6E
Interpretation Introduction

Interpretation:

To show that fixed points for the averaged system correspond to phase-locked periodic solutions for the original forced oscillator. Show further that saddle-node bifurcations of fixed points for the averaged system correspond to saddle-node bifurcation of cycles for the oscillator.

Concept Introduction:

In two-dimensional system, there are four common ways in which limit cycles are created or destroyed.

Global bifurcations are harder to detect because they involve large regions of the phase plane rather than just the neighborhood of a single fixed point.

A bifurcation in which two limit cycles annihilateandcoalesceis called a fold or saddle-node bifurcation of cycles.

At the bifurcation, the cycle touches thesaddle point and becomes a homoclinic orbit. Then it is called as saddle-loop or homoclinic bifurcation.

Bifurcation: it is defined as the point area at which something is divided into two parts and branch. The point in the system equation at which bifurcating occurs.

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Function: y=xsinx Interval: [ 0 ; π ] Requirements: Draw the graphical form of the function. Show the coordinate axes (x and y). Choose the scale yourself and show it in the flowchart. Create a flowchart based on the algorithm. Write the program code in Python. Additional requirements: Each stage must be clearly shown in the flowchart. The program must plot the graph and save it in PNG format. Write the code in a modular way (functions and main section should be separate). Expected results: The graph of y=xsinx will be plotted in the interval [ 0 ; π ]. The algorithm and flowchart will be understandable and complete. When you test the code, a graph file in PNG format will be created.
PLEASE SOLVE STEP BY STEP WITHOUT ARTIFICIAL INTELLIGENCE OR CHATGPT SOLVE BY HAND STEP BY STEP
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