  In this paper, we establish a result of Lagrangian controllability for a
fluid at low Reynolds number, driven by the stationary Stokes equation. This
amounts to the possibility of displacing a part of a fluid from one zone to
another by suitably using a boundary control. This relies on a weak variant of
the Runge-Walsh's theorem (on approximation of harmonic functions) concerning
the Stokes equation. We give two variants of this result, one of which we
believe to be better adapted to numerical simulations.
