A Variational Level Set Approach to Multiphase Motion
โ Scribed by Hong-Kai Zhao; T. Chan; B. Merriman; S. Osher
- Publisher
- Elsevier Science
- Year
- 1996
- Tongue
- English
- Weight
- 433 KB
- Volume
- 127
- Category
- Article
- ISSN
- 0021-9991
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โฆ Synopsis
The point at which they meet (the triple junction) has prescribed angles which can be shown [12] to be defined by A coupled level set method for the motion of multiple junctions (of, e.g., solid, liquid, and grain boundaries), which follows the gradient flow for an energy functional consisting of surface tension (proportional to length) and bulk energies (proportional to area), is
Our objective here is to develop and implement numerithe theory as given in [12]. Other applications of this methocal algorithms which ''capture'' rather than ''track'' the dology, including the decomposition of a domain into subregions interfaces, based on the level set method of Osher and with minimal interface length, are discussed. Finally, some new Sethian [9]. The usual advantages of the level set method techniques and results in level set methodology are presented.
๐ SIMILAR VOLUMES
A coupled level set method for the motion of multiple junctions is proposed. The new method extends the "Hamilton-Jacobi" level set formulation of Osher and Sethian. It retains the feature of tracking fronts by following level sets and allows the specification of arbitrary velocities on each front.
The level-set method has been successfully applied to a variety of problems that deal with curves in R 2 or surfaces in R 3 . We present here a combination of these two cases, creating a level-set representation for curves constrained to lie on surfaces. We study primarily geometrically based motion
The level set method was originally designed for problems dealing with codimension one objects, where it has been extremely succesful, especially when topological changes in the interface, i.e., merging and breaking, occur. Attempts have been made to modify it to handle objects of higher codimension
where (x, y, z, t) is the vorticity vector and v(x, y, z, t) is the velocity vector. We present an Eulerian, fixed grid, approach to solve the motion of an incompressible fluid, in two and three dimensions, in which In a vortex sheet, is a singular measure concentrated the vorticity is concentrate