... M in an infinite vol ume of an ideal incompressible fluid; inside the body, a point ... sin u= · a1 = M + 1 + m , m b= = , m · · , · M + 2 + m , m 2 y .. (, ) m O1 (2) O ...
... Ramodanov, S. M., Tenenev, V. A., and Treschev, D. V., Self-propulsion of a Body with Rigid Surface and Variable Coefficient of ... Chaotic Dyn., 2012, vol. 17, no. 6, pp. 547558. 30. ...
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... revised 14 April 2014 Accepted for publication 17 April 2014 Published 28 May 2014 ... Motion of Vortex Rings (London: Macmillan) Abramowitz M and Stegun I A 1972 Handbook ...
... represented in the form [2, 10] M = M в , = - в , = A(M + Z ), (AM , ) , A = diag(A1 ... M , it can b e rewritten using the undetermined multipliers as F0 F2 E = 1 + 1 , MM ...
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... Tomita, H., Sano, M. M., Yoshida, T., and Ebisuzaki, T., Dynamics of Two-Sign Point Vortices in Positive and Negative Temperature State, Phys. Rev. Lett., 2005, vol. 94, 054502, 4 pp. ...
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... 1 2006 ON THE FALL OF A HEAVY RIGID BODY IN AN IDEAL FLUID S27 Fig. 1. 1.3. Plane-parallel motion [5, 9, 17, 20]. ... The plane-parallel motion of a rigid b o dy is determined by the invariant relations M 1 = M2 = 0, 3 = 3 = 0. ...