In eutectic alloys solidified in a thermal gradient, it has been obser
ved that the final shape of the grains nucleated in the bulk of the li
quid is more elongated in the direction opposite to that of the heat f
low. This experimental result appears to be in contradiction with that
expected for the growth of an isolated grain, since the portion of th
e interface located in the downstream heat flow direction is the most
undercooled and thus has the highest growth rate. However, when consid
ering a family of grains which continuously nucleate in the bulk of th
e liquid, it is shown that the impingement of the grains limits their
growth in the downstream heat flow direction and thus explains their f
inal shape. In order to investigate this phenomenon, the differential
equation which governs the growth of an isolated eutectic grain in a t
hermal gradient has been derived and solved analytically for the two e
xtreme positions of the interface along the heat flow direction. Using
these relationships, the asymmetry factor of the grains has been dedu
ced as a function of the solidification parameters. The overall shape
of an isolated grain has also been predicted using numerical integrati
on. Finally, these results are integrated into a stochastic model of g
rain structure formation and the simulated microstructure is compared
with experimental micrographs previously obtained for hypereutectic al
uminium-silicon alloys remelted by laser.