Since the time of surfaces -+ in differential Gauss, parametrized (x, y) P(x, y) have been described a frame attached to the moving geometry through TI(x, y) surface. One introduces the Gauss- which linear dif- Weingarten equations are, ferential equations = U = TIX T1, VT', PY (1. for the and their condition frame, compatibility - = V + U, V] 0, UY (1.2) which the Gauss-Codazzi For surfaces in three-dim- represents equations . a sional Euclidean the frame T1 lies in the usually or space, group SO(3) SU(2). On the other a of a non-linear in the form hand, representation equation (1.2) is...
Since the time of surfaces -+ in differential Gauss, parametrized (x, y) P(x, y) have been described a frame attached to the moving geometry through T...
This is one of the first books on a newly emerging field of discrete differential geometry and an excellent way to access this exciting area. It surveys the fascinating connections between discrete models in differential geometry and complex analysis, integrable systems and applications in computer graphics.
The authors take a closer look at discrete models in differential
geometry and dynamical systems. Their curves are polygonal, surfaces
are made from triangles and quadrilaterals, and time is discrete.
Nevertheless, the difference between...
This is one of the first books on a newly emerging field of discrete differential geometry and an excellent way to access this exciting area. It su...
