... 70F35, 82C22 REGULAR AND CHAOTIC DYNAMICS, V. 8, 4, 2003 431 V. V. KOZLOV, M. Yu ... with resp ect REGULAR AND CHAOTIC DYNAMICS, V. 8, 4, 2003 433 V. V. KOZLOV, M. Yu ... REGULAR AND CHAOTIC DYNAMICS, V. 8, 4, 2003 435 V. V. KOZLOV, M. Yu. ...
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Ссылки http://ics.org.ru/upload/iblock/d40/126-galton-board_ru.pdf -- 2035.7 Кб -- 28.10.2015 Похожие документы
... n xi (2 ) xi Hence f1 = m W + (u). (2 )n (7.8) The function should be chosen from the condition f1 dx du = 0. ... Then the second variation of the potential energy (the third term in (8.2)) is equal to km mm . ...
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Ссылки http://ics.org.ru/upload/iblock/c96/169-the-vlasov-kinetic-equation-dynamics-of-continuum-and-turbulence_ru.pdf -- 325.0 Кб -- 28.10.2015 Похожие документы
... 5.8) It is well known that if m = n and the functions (5.1) are pairwise in ... classical result to the case m > n. The differential 1-form (5.8) is = Uk +1 dx k+1 ...
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Ссылки http://ics.org.ru/upload/iblock/250/188-an-extended-hamilton-jacobi-method_ru.pdf -- 217.5 Кб -- 28.10.2015 Похожие документы
... the joint four-dimensional level of the integrals (M , ) = c = const, 2 = 1 (4.8) by Andoyer variables (L, G, l, g ) and fix ... The values of the system parameters are A = diag(1.8, 1.5, 2), C = diag(0.5, 2.9, 1.4), µ = 1, (M , ) = 1, E0 = 7. ...