  We discuss a generic mechanism for shear-thickening analogous to
entropy-driven phase reentrance. We implement it in the context of
non-relaxational mean-field glassy systems: although very simple, the
microscopic models we study present a dynamical phase diagram with second and
first order stirring-induced jamming transitions leading to intermittency,
metastability and phase coexistence as seen in some experiments. The jammed
state is fragile with respect to change in the stirring direction. Our approach
provides a direct derivation of a Mode-Coupling theory of shear-thickening.
