In the context of the energy landscape description of supercooled liquids,
we propose an explanation for the different behaviour of fragile and strong
liquids. Above Goldstein's temperature T-x, diffusion is interpreted as mo
tion in the phase space among saddles of the potential energy. Two mechanis
ms of diffusion then rise: mechanism A takes place when the system overcome
s potential-energy barriers long stable uphill directions, while mechanism
B consists in finding unstable downhill directions out of saddle. Depending
on the mutual efficiency of A and B, the usual classification of liquids i
n fragile and strong is recovered. Moreover, this scenario naturally predic
ts the possibility of fragile-to-strong crossover when lowering the tempera
ture.