In this work we perform an analysis of the onset of chaos in mean-fiel
d dynamics in the presence of volume instabilities. As a main finding,
we show that the mean-field evolution presents two different regimes:
a first one dominated by the almost decoupled amplification of severa
l collective unstable modes, leading to the early condensation of the
system into clusters, which is followed by a second stage dominated by
a coalescence mechanism among the large-density domains. Finally we s
how that, even at the latest stage considered, chaos does not appear a
s fully developed since a hierarchy of the different unstable modes, i
nherited from the initial regular amplification of instabilities, rema
ins.