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Orbit (control theory) : ウィキペディア英語版
Orbit (control theory)

The notion of orbit of a control system used in mathematical control theory is a particular case of the notion of orbit in group theory.
==Definition==
Let
\dot q=f(q,u)
be a \ ^\infty control system, where

belongs to a finite-dimensional manifold \ M and \ u belongs to a control set \ U. Consider the family =\
and assume that every vector field in is complete.
For every f\in and every real \ t, denote by \ e^ the flow of \ f at time \ t.
The orbit of the control system \dot q=f(q,u) through a point q_0\in M is the subset _ of \ M defined by
:_=\ f_}\circ\cdots\circ e^(q_0)\mid k\in\mathbb,\ t_1,\dots,t_k\in\mathbb,\ f_1,\dots,f_k\in\}.
;Remarks
The difference between orbits and attainable sets is that, whereas for attainable sets only forward-in-time motions are allowed, both forward and backward motions are permitted for orbits.
In particular, if the family is symmetric (i.e., f\in if and only if -f\in ), then orbits and attainable sets coincide.
The hypothesis that every vector field of is complete simplifies the notations but can be dropped. In this case one has to replace flows of vector fields by local versions of them.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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