Capillary surfaces are closely related to minimal surfaces. In
fact, capillary surfaces minimize a more general functional than
do minimal surfaces. The standard mathematical model for volume
constrained capillary problems is as follows: a set
in
is the region occupied by one of the fluids, which
contacts a fixed surface
. In micro-gravity (i.e.,
gravity is negligible) the energy functional is

where
is the free surface of
(i.e., that
portion of
which is not contained in
),
is the portion of
which is wetted by
(i.e.,
), and
is a constant
depending on the materials involved. We seek local minima of this
energy functional if
is required to satisfy a volume
constraint, that is, we only consider volume conserving
perturbations. The first variation yields that the mean curvature
of
is a constant H, and that the angle between the
normal to
and the normal to
along the curve of
contact is
, at least when
is
smooth enough to have a normal. A surface satisfying this first
order condition is called stationary. If gravity is included, the mean curvature is an affine function of height, but the contact angle condition remains the same.
For anyone interested in looking at these surfaces, Finn's book is a good place to start.