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Topological Changes

When different parts of a surface collide, a topological change must be made. For simplicity, we make the assumption that if is a normal to , then so is . The collision is thus between oppositely oriented segments (since segments bound solids and/or ``outside'' regions); as a limiting case, two corners may collide, in which case either pair of oppositely oriented normals could be used. If one facet completely overlaps the opposite, the shorter facet is completely removed, as is the section of the longer facet that overlaps the shorter. Then the remaining portions of the longer facet are connected to the neighbors of the shorter one. If the opposing facets only partially overlap, then the portion of overlap is removed from both facets, and the remaining piece is attached to the loose former neighbor of the other facet.

This cutting and pasting will produce bad corners, i.e. ones which omit normals of the Wulff shape (unless is a parallelogram). These illegal corners will have infinite chemical potential and are places where zero-length facets must be inserted until none of the normals of between neighboring edges are omitted. These new edges will move with initially infinite velocity, although the velocity will immediately become finite as the edges become of non-zero length. it remains to be shown that there is indeed an unique evolution in SD or in SALK out of such a corner.

In SALK it is possible for an entire connected component to shrink to a point if there is more than one component surrounded by the same transport medium. If this occurs, all its edges are simultaneously removed. The total average curvature, which is the chemical potential in the transport medium, drops by an amount equal to the length of the boundary of (or some weighted sum of the if the are not all equal to 1).



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