Discrete Willmore Flow
Alexander Bobenko and Peter Schröder
Discrete Willmore Flow Alexander Bobenko and Peter Schrder Goals of - - PowerPoint PPT Presentation
Discrete Willmore Flow Alexander Bobenko and Peter Schrder Goals of Paper Present a technique for smoothing surfaces Advance idea of discrete geometry vs. discretizations of continuous geometry Willmore Energy 2 K dA = 1 E w
Alexander Bobenko and Peter Schröder
Present a technique for smoothing surfaces Advance idea of discrete geometry vs.
K: Gaussian curvature= k1k2 k1, k2: are principle curvatures
E ws=H
2KdA= 1
4k1k2
2dA
– Mostly just scale invariance that counts
Minimizing energy minimizes k1
2+k2 2
Special case of physics for thin structures Fourth order flow—allows G1 boundary conditions
E ws=H
2KdA= 1
4k1k2
2dA
Traditional approach
– Finite elements or finite differences – Lose many of the guarantees of the continuous – Finite elements are well understood
Alternative
– Formulate discrete analogs – Respect symmetries/invariants
Yoshizawa and Belyaev
– Integrand not always positive E ws=H
2K dA= 1
4k1k2
2dA
Formulated for 2-manifolds with boundary
Positive Zero if points lie on a sphere
eij
j
i 2
Let D
be a triangulated neighborhood of a
R is independent of curvatures R1 R=1 if two edges align with curvature lines
lim W D W sD=R
Nice formulations of derivatives to reduce system
Can handle singularities due to cocircular points
– Uses Möbius invariance
G1
– Fixed positions and normals – Not necessarily on boundaries
Free
– Add a point at infinity per boundary – Extra terms in energy:
Angle between boundary edges (3)
Forward Euler
– Small timesteps
Backward Euler
– Nonlinear system
In practice
– Linearize gradient – L is nxn with an entry per row per neighbor 1 t ILt xt=Et
24 steps
Error analysis and convergence analysis Convergence to lines of curvature
– Extend to quads