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Lagrange stability is a concept in the stability theory of dynamical systems, named after Joseph-Louis Lagrange. Consider a real continuous dynamical system , where is . For any point in the state space, , the motion is said to be ''positively Lagrange stable'' if the positive semi-orbit is comapct. If the negative semi-orbit is comapct, then the motion is said to be ''negatively Lagrange stable''. The motion through is said to be ''Lagrange stable'' if it is both positively and negatively Lagrange stable. If the state space is the Euclidean space , then the above definitions are equivalent to and being bounded, respectively. A dynamical system is said to be positively-/negatively-/Lagrange stable if ''for each'' , the motion 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)』 ■ウィキペディアで「Lagrange stability」の詳細全文を読む スポンサード リンク
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