BALL-MAP: HOMEOMORPHISM BETWEEN COMPATIBLE SURFACES
Author(s) -
Frédéric Chazal,
André Lieutier,
JAREK ROSSIGNAC,
Brian Whited
Publication year - 2010
Publication title -
international journal of computational geometry and applications
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.221
H-Index - 39
eISSN - 1793-6357
pISSN - 0218-1959
DOI - 10.1142/s021819591000330x
Subject(s) - mathematics , diffeomorphism , bijection , ball (mathematics) , homeomorphism (graph theory) , isotopy , combinatorics , geometry , pure mathematics
Homeomorphisms between curves and between surfaces are fundamental to many applications of 3D modeling, graphics, and animation. They define how to map a texture from one object to another, how to morph between two shapes, and how to measure the discrepancy between shapes or the variability in a class of shapes. Previously proposed maps between two surfaces, S and S′, suffer from two drawbacks: (1) it is difficult to formally define a relation between S and S′ which guarantees that the map will be bijective and (2) mapping a point x of S to a point x′ of S′ and then mapping x′ back to S does in general not yield x, making the map asymmetric. We propose a new map, called ball-map, that is symmetric. We define simple and precise conditions for the ball-map to be a homeomorphism. We show that these conditions apply when the minimum feature size of each surface exceeds their Hausdorff distance. The ball-map, BMS,S′, between two such manifolds, S and S′, maps each point x of S to a point x′ = BMs,s′(x) of S′. BMS′,S is the inverse of BMS,S′, hence BM is symmetric. We also show that, when S and S′ are Ck (n - 1)-manifolds in ℝn, BMS,S′ is a Ck-1 diffeomorphism and defines a Ck-1 ambient isotopy that smoothly morphs between S to S′. In practice, the ball-map yields an excellent map for transferring parameterizations and textures between ball compatible curves or surfaces. Furthermore, it may be used to define a morph, during which each point x of S travels to the corresponding point x′ of S′ along a broken line that is normal to S at x and to S′ at x′.
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