Аннотация:
We study a mechanical system that consists of a 2D rigid body interacting
dynamically with two point vortices in an unbounded volume of an incompressible, otherwise
vortex-free, perfect fluid. The system has four degrees of freedom. The governing equations can
be written in Hamiltonian form, are invariant under the action of the group $E(2)$ and thus, in
addition to the Hamiltonian function, admit three integrals of motion. Under certain restrictions
imposed on the system’s parameters these integrals are in involution, thus rendering the system
integrable (its order can be reduced by three degrees of freedom) and allowing for an analytical
analysis of the dynamics.