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Physical models of area-minimizing minimal surfaces can be made by dipping a wire frame into a soap solution, forming a soap film, which is a minimal surface whose boundary is the wire frame.
Recent work in minimal surfaces has identified new completely embedded minimal surfaces, that is minimal surfaces which do not intersect. In particular Costa's minimal surface was first described mathematically in 1982 by Celso Costa and later visualized by Jim Hoffman. This was the first such surface to be discovered in over a hundred years. Jim Hoffman, David Hoffman and William Meeks III, then extended the definition to produce a family of surfaces with different rotational symmetries.
Minimal surfaces have become an area of intense mathematical and scientific study over the past 15 years, specifically in the areas of molecular engineering and materials science, due to their anticipated nanotechnology applications.
In the art world, minimal surfaces have been extensively explored in the sculpture of Robert Engman (1927- ), Robert Longhurst (1949 - ), Charles O. Perry (1929 - ), among others.
The term "minimal surface" is because these surfaces originally arose as surfaces that minimized surface area, subject to some constraint, such as total volume enclosed or a specified boundary, but the term is used more generally.
Minimal surfaces are the critical points for the mean curvature flow: these are both characterized as surfaces with vanishing mean curvature.
The definition of minimal surfaces can be generalized/extended to cover constant mean curvature surfaces: surfaces with a constant mean curvature, which need not equal zero.
Category:Differential geometry Category:Differential geometry of surfaces
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