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Lagrange stability
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Lagrange stability : ウィキペディア英語版
Lagrange stability

Lagrange stability is a concept in the stability theory of dynamical systems, named after Joseph-Louis Lagrange.
Consider a real continuous dynamical system (T,M,\Phi), where T is \mathbb. For any point in the state space, x \in M , the motion \Phi(t,x) is said to be ''positively Lagrange stable'' if the positive semi-orbit \gamma_x^+ is comapct. If the negative semi-orbit \gamma_x^- is comapct, then the motion is said to be ''negatively Lagrange stable''. The motion through x is said to be ''Lagrange stable'' if it is both positively and negatively Lagrange stable. If the state space M is the Euclidean space \mathbb^n, then the above definitions are equivalent to \gamma_x^+, \gamma_x^- and \gamma_x being bounded, respectively.
A dynamical system is said to be positively-/negatively-/Lagrange stable if ''for each'' x \in M , the motion \Phi(t,x) is positively-/negativey-/Lagrange stable, respectively.
==Further reading==

* Elias P. Gyftopoulos, ''Lagrange Stability and Liapunov's Direct Method''. Proc. of Symposium on Reactor Kinetics and Control, 1963. ((PDF ))
*


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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