Mode interaction between odd and even modes in two-dimensional Boussin
esq convection in a box is revisited. It is noted that in the large as
pect ratio limit the structure of the amplitude equations depends on t
he boundary conditions applied at the sidewalls, however distant. With
no-slip sidewall boundary conditions the equations approach those for
an unbounded layer with periodic boundary conditions; this is not the
case for free-slip boundary conditions. Thus only in the former case
can the large aspect ratio system be considered a small perturbation o
f the unbounded system. The reasons for the different large aspect rat
io limits are traced to the presence of ''hidden'' symmetries in the s
tress-free case. Homotopic continuation is used to extend these result
s to other types of boundary conditions.