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In mathematics, in the study of dynamical systems, an orbit is a collection of points related by the evolution function of the dynamical system. The orbit is a subset of the phase space and the set of all orbits is a partition of the phase space, that is different orbits do not intersect in the phase space. Understanding the properties of orbits by using topological method is one of the objectives of the modern theory of dynamical systems. ## Definition

### Real dynamical system

### Notes

### Examples

## Stability of orbits

## See also

## References

For discrete-time dynamical systems the orbits are sequences, for real dynamical systems the orbits are curves and for holomorphic dynamical systems the orbits are Riemann surfaces.

Given a dynamical system (T, M, Φ) with T a group, M a set and Φ the evolution function

- $Phi:\; T\; times\; M\; to\; M$

we define

- $I(x):=\{t\; in\; T\; :\; (t,x)\; in\; T\; times\; M\; \},$

then the set

- $gamma\_x:=\{Phi(t,x)\; :\; t\; in\; I(x)\}$

is called orbit through x. An orbit which consists of a single point is called constant orbit. A non-constant orbit is called closed or periodic if there exists a t in T so that

- $Phi(t,\; x)\; =\; x$

Given a real dynamical system (R, M, Φ), I(x) is an open interval in the real numbers, that is $I(x)\; =\; ]t\_x^-\; ,\; t\_x^+[$. For any x in M

- $gamma\_\{x\}^\{+\}\; :=\; \{Phi(t,x)\; :\; t\; in\; ]0,t\_x^+[\}$

- $gamma\_\{x\}^\{-\}\; :=\; \{Phi(t,x)\; :\; t\; in\; ]t\_x^-,0[\}$

It is often the case that the evolution function can be understood to compose the elements of a group, in which case the group-theoretic orbits of the group action are the same thing as the dynamical orbits.

- The orbit of a equilibrium point is a constant orbit

A basic classification of orbits is

- constant orbits or fixed points
- periodic orbits
- non-constant and non-periodic orbits

An orbit can fail to be closed in two interesting ways. It could be an asymptotically periodic orbit if it converges to a periodic orbit. Such orbits are not closed because they never truly repeat, but they become arbitrarily close to a repeating orbit. An orbit can also be chaotic. These orbits come arbitrarily close to the initial point, but fail to ever converge to a periodic orbit. They exhibit sensitive dependence on initial conditions, meaning that small differences in the initial value will cause large differences in future points of the orbit.

There are other properties of orbits that allow for different classifications. An orbit can be hyperbolic if nearby points approach or diverge from the orbit exponentially fast.

- Wandering set
- Phase space method
- Cobweb plot or Verhulst diagram
- Periodic points of complex quadratic mappings and multiplier of orbit

- Anatole Katok and Boris Hasselblatt (1996).
*Introduction to the modern theory of dynamical systems*. Cambridge. ISBN 0-521-57557-5.

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Last updated on Sunday August 17, 2008 at 14:50:16 PDT (GMT -0700)

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This article is licensed under the GNU Free Documentation License.

Last updated on Sunday August 17, 2008 at 14:50:16 PDT (GMT -0700)

View this article at Wikipedia.org - Edit this article at Wikipedia.org - Donate to the Wikimedia Foundation

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