![Nonlinear Dynamics and Chaos](https://www.bartleby.com/isbn_cover_images/9780429972195/9780429972195_largeCoverImage.gif)
Concept explainers
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.
![Check Mark](/static/check-mark.png)
Want to see the full answer?
Check out a sample textbook solution![Blurred answer](/static/blurred-answer.jpg)
Chapter 8 Solutions
Nonlinear Dynamics and Chaos
- y = log 5 – x2 - 4 00arrow_forwardPlease fill in the rest of the steps of the proof of Thm 2.5. Show how "Repeating this step with n-1,n-2,...,2 in place of n" gives us the desired result.arrow_forwardConsider the initial value problem y"+y'-12y= 0, y(0) = a, y'(0) = 4 Find the value of a so that the solution to the initial value problem approaches zero as too a =arrow_forward
- Linear Algebra: A Modern IntroductionAlgebraISBN:9781285463247Author:David PoolePublisher:Cengage Learning
![Text book image](https://www.bartleby.com/isbn_cover_images/9781285463247/9781285463247_smallCoverImage.gif)