Relaxing Hele-Shaw Boundary Motion


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 ××=-²² 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

Further reading can be found in:

James Blowey