The Hele-Shaw problem is: find
satisfying
²
=0 where
x
\
(t)
with
[
]-+=-2V,
=-
where
x
(t)
where
represents the temperature in a bounded region,
,
V×n is the normal velocity of
(t) into the
liquid region n is
the unit normal pointing pointing into the liquid region
[.]-+
denotes the difference in the limits of the quantity in the brackets
as x tends to
(t) from each side and
is the
sum of the principal curvatures
(t) (with the convention
that
is positive when the solid region is convex).
This is a very difficult problem to solve. By relaxing this problem and
considering the Cahn-Hilliard equation
ut-
=0, x
× ¼ ×
×
=-
²
² u+
'(u), x
where
(.) is a double well potential function. It is possible
to formally show that in the limit as
goes to 0 the problem
converges to the solution of the Hele-Shaw problem.
Below is a numerical simulation with the white lines representing the
level set
(t) as time evolves