All equations with Poisson brackets are tested with symbolic features of the Maple system. This variant of Hamilton formalism easily spreads in the case of arbitrary number of magnetically interactive symmetric tops. Conservation laws following from the system symmetry are considered. Such an approach allows the equations to be represented in the galilei-invariant vector form in contrast to default definition in Euler's angl es. Hamilton motion equations are obtained on the basis of Poisson structure in the dynamic variables area. The task requires the development of the classic Hamilton formalism for the systems of magnetically interactive bodies, including the systems of magnets and/or superconductive magnets (mixed sys- tems). system, notwithstandi ng that force is non-central. Since the energy of interaction depends only on the relative position of the bodies, then the considera- tion is too much simplified in the c.m.
The general form of the interaction energy is discovered for the case of coincidence of mass and magnetic symmetries. The model of inter- action is built on quasi-stationary approach for electroma gnetic field, and symmetric tops with different moments of inertia of the bodies are considered. Dynamics of two bodies, which interact by magnetic forces, is considered.
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