Projective vector field: Difference between revisions

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[[Image:DuffingMap.png|right|thumb|Plot of the Duffing map showing chaotic behavior, where ''a''&nbsp;=&nbsp;2.75 and ''b''&nbsp;=&nbsp;0.15.]]
[[Image:Tw duffing.png|right|thumb|[[Phase portrait]] of a two-well Duffing oscillator (a differential equation, rather than a map) showing chaotic behavior.]]
The '''Duffing map''' (also called as 'Holmes map') is a [[discrete-time]] [[dynamical system]]. It is an example of a dynamical system that exhibits [[chaos theory|chaotic behavior]].  The Duffing [[function (mathematics)|map]] takes a point (''x<sub>n</sub>'',&nbsp;''y<sub>n</sub>'') in the [[plane (mathematics)|plane]] and maps it to a new point given by
:<math>x_{n+1}=y_n\,</math>
:<math>y_{n+1}=-bx_n+ay_n-y_n^3.\,</math>
 
The map depends on the two [[constant (mathematics)|constant]]s ''a'' and ''b''. These are usually set to ''a''&nbsp;=&nbsp;2.75 and ''b''&nbsp;=&nbsp;0.2 to produce chaotic behaviour. It is a discrete version of the [[Duffing equation]].
 
==References==
{{reflist}}
 
== External links ==
* [http://scholarpedia.org/article/Duffing_oscillator Duffing oscillator on Scholarpedia]
 
{{Chaos theory}}
 
[[Category:Chaotic maps]]
 
{{Mathapplied-stub}}

Revision as of 22:07, 18 May 2013

Template:No footnotes

File:DuffingMap.png
Plot of the Duffing map showing chaotic behavior, where a = 2.75 and b = 0.15.
Phase portrait of a two-well Duffing oscillator (a differential equation, rather than a map) showing chaotic behavior.

The Duffing map (also called as 'Holmes map') is a discrete-time dynamical system. It is an example of a dynamical system that exhibits chaotic behavior. The Duffing map takes a point (xnyn) in the plane and maps it to a new point given by

The map depends on the two constants a and b. These are usually set to a = 2.75 and b = 0.2 to produce chaotic behaviour. It is a discrete version of the Duffing equation.

References

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External links

Template:Chaos theory

Template:Mathapplied-stub