Magnetoconvection in the Sun does not take place in the idealized situ
ation in which the imposed field is vertical or horizontal. Instead, f
ields in sunspots and other active region features are inclined to the
vertical, and so the system does not possess the left-right symmetry
that is a feature of many analytical and numerical studies. As a first
step toward the understanding of convection in general field configur
ations, we consider the nonlinear behavior of compressible convection
in the presence of a uniform, externally imposed, oblique magnetic hel
d. Numerical simulations demonstrate that all solutions take the form
of traveling waves, regardless of the degree of nonlinearity or field
intensity, for angles of obliquity 0 < phi < pi/2. However, the struct
ure of the convection cells, their wave speed, and direction depend se
nsitively upon the degree of nonlinearity, field angle, and field stre
ngth. For sufficiently vigorous convection, we find that all solutions
have a net horizontal velocity at the upper surface of the computatio
nal domain that is in the direction of the field tilt from vertical (w
hereas the total horizontal momentum is zero). In cases where the conv
ection dominates over the magnetic field, we find the waves propagatin
g in the same direction as the net surface velocity but with phase vel
ocities that are typically an order of magnitude smaller. In cases whe
re the field dominates over the convection, we find a similar relation
in speeds but with waves propagating in the opposite direction. The r
esults appear to be qualitatively independent of the precise boundary
conditions applied to the field, as long as the latter do not impart a
net horizontal momentum to the layer.