A dynamical system is a set $M$ equipped with some geometric structure (say a manifold) together with a law of motion, that is the law of evolution of points which is the action
The parameter of evolution is called time. If the law of evolution is translation invariant we say that the dynamical system is autonomous.
The law of motion is often given by (what is in a particular case) an equivalent datum, e.g. by an initial value problem for a differential equation “of evolution type”.
Sometimes the evolution is only partially defined; this is most often in dynamical systems induced by evolution differential equations which do not necessarily have existence of solutions for arbitrary large time, or the dynamical system is defined only for nonnegative time.
Sometimes time is taken to be discrete, that is belonging to integers $\mathbb{Z}$ or say to positive integers $\mathbb{N}$. The autonomous discrete dynamical system is determined by the morphism $S: M\to M$, sometimes called shift which determines the change from time $n$ to $n+1$. The autonomous dynamical systems can be viewed in quite general categories in which there are nontrivial endomorphisms; so one has complex dynamics, algebraic dynamics, arithmetic dynamics and so on.
Most often one looks at dynamical systems in which $M$ is a smooth manifold. Dynamical systems are used to describe not only physical motions but also the behaviour of parameters of various systems, e.g. in sociological, financial, weather and other models.
See also
Discussion in terms of category theory:
William Lawvere, Functional Remarks on the General Concept of Chaos , IMA reprint 87, 1984 (pdf)
George Dimitrov, Fabian Haiden, Ludmil Katzarkov, Maxim Kontsevich, Dynamical systems and categories, arxiv/1307.8418
Last revised on May 27, 2019 at 14:13:06. See the history of this page for a list of all contributions to it.