... M c 2 1 = m - M 3 , 3 2 3 2 1/2 M1 = m = const, c 2 = k 2 - 1 m2 - m + M 2 3 , 3 ... M , ) (L, s) (its square is equal to identity), found by A. I. Dokshevich: L1 = - L2 ... of the moment on semimoving axes S1 = M 1 1 + M 2 2 , 266 S3 = M 1 2 - M 2 1 ...
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... Systems, 1988, vol. 8/8*, no. 9. 21. Conley, Ch., ... Tomita, H., Sano, M. M., Yoshida, T., and Ebisuzaki, T., Dynamics of Two-Sign Point Vortices in Positive and Negative ...
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... is found from the condition (E, )· = 0: = ( I в + M Q, I E ) ( E, I Q E ) 1 1 Fig ... 8. G. K. Suslov, Theoretical Mechanics (Gostekhizdat, Moscow, 1946) [in Russian]. ...
... M. A. Strem · Application R. J. Adrian of the nature of stirring with three ... Liu, R. H., Sharp, K. V., Olsen, M. G., Stremler, M. A., Santiago, J. G., Adrian, R ... Beeb e, D. J., Adrian, R. J., Olsen, M. G., Stremler, M. A., Aref, H., and Jo, B. H ...
... m = (m1 , m2 , m3 ) and Е = (Е1 , Е2 , Е3 ) are related to the momentum and ... functions, m = (m, m), Е = (Е, Е), (51) and have a rank of eight (provided that m ... m = (m, m), Thus, we ultimately conclude that 1. if m , Е = 0, equations (100 ...
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