Cosmic Research, Vol. 42, No. 5, 2004, pp. 489ґ534. Translated from Kosmicheskie Issledovaniya, Vol. 42, No. 5, 2004, pp. 509ґ554. Original Russian Text Copyright ? 2004 by Panasyuk, Kuznetsov, Lazutin, Avdyushi, Alexeev, Ammosov, Antonova, Baishev, Belenkaya, Beletsky, Belov, Benghin, Bobrovnikov, Bondarenko, Boyarchuk, Veselovsky, Vyushkova, Gavrilieva, Gaidash, Ginzburg, Denisov, Dmitriev, Zherebtsov, Zeleny, Ivanov-Kholodny, Kalegaev, Kanonidi, Kleimenova, Kozyreva, Kolomiitsev, Krasheninnikov,

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... The optimal control, which led oscillatory system to a certain energy level from any initial conditions at minimum time, is found. ... A set of points where the trajectory becomes an arc of a circle with the other center is called the switching line. ... For drawing switching line near the origin (see for example Figure 3) we note from the system (1) that time is proportional to the sum of the angles 214 this sums for optimal and quasi-optimal processes. ... The control function (14) is not optimal....

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... Another situation is that of effective slip, beff , which refers to a situation where slippage at a complex heterogeneous surface is evaluated by averaging of a flow over the length scale of the experimental configuration (e.g. a channel etc) [3, 14ґ16]. ... Rough surfaces 4. ... We seek the solution for a velocity u by perturbation analysis: u = u0 + u1 , (6) where u0 is the velocity of the Poiseuille flow, and the effective slip length beff at the super-hydrophobic surface is defined as b Figure 6...

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