Abstract
The existence of a maximal global attractor is demonstrated for the dynamical system generated by the initial boundary value problem associated with the motion of a non-linear bipolar fluid; the attractor has the form A=∩t>0S(t)Bρ′(H2(Ω))3 where S(t) is the relevant non-linear semigroup and Bρ′(H2(Ω))3 (the ball of radius ρ′>0 in (H2(Ω))3) is, for ρ′ sufficiently large, an absorbing set. Upper bounds are obtained for the Hausdorff and Fractal dimensions of the attractor A.
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