Catenoid

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Template:Short description

three-dimensional diagram of a catenoid
A catenoid
animation of a catenary sweeping out the shape of a catenoid as it rotates about a central point
A catenoid obtained from the rotation of a catenary

In geometry, a catenoid is a type of surface, arising by rotating a catenary curve about an axis (a surface of revolution).[1] It is a minimal surface, meaning that it occupies the least area when bounded by a closed space.[2] It was formally described in 1744 by the mathematician Leonhard Euler.

Soap film attached to twin circular rings will take the shape of a catenoid.[2] Because they are members of the same associate family of surfaces, a catenoid can be bent into a portion of a helicoid, and vice versa.

Geometry

The catenoid was the first non-trivial minimal surface in 3-dimensional Euclidean space to be discovered apart from the plane. The catenoid is obtained by rotating a catenary about its directrix.[2] It was found and proved to be minimal by Leonhard Euler in 1744.[3][4]

Early work on the subject was published also by Jean Baptiste Meusnier.[5][4]Template:Rp There are only two minimal surfaces of revolution (surfaces of revolution which are also minimal surfaces): the plane and the catenoid.[6]

The catenoid may be defined by the following parametric equations: x=ccoshvccosuy=ccoshvcsinuz=v where u[π,π) and v and c is a non-zero real constant.

In cylindrical coordinates: ρ=ccoshzc, where c is a real constant.

A physical model of a catenoid can be formed by dipping two circular rings into a soap solution and slowly drawing the circles apart.

The catenoid may be also defined approximately by the stretched grid method as a facet 3D model.

Helicoid transformation

Continuous animation showing a right-handed helicoid deforming into a catenoid, a left-handed helicoid, and back again
Deformation of a right-handed helicoid into a left-handed one and back again via a catenoid

Because they are members of the same associate family of surfaces, one can bend a catenoid into a portion of a helicoid without stretching. In other words, one can make a (mostly) continuous and isometric deformation of a catenoid to a portion of the helicoid such that every member of the deformation family is minimal (having a mean curvature of zero). A parametrization of such a deformation is given by the system x(u,v)=sinθcoshvcosu+cosθsinhvsinuy(u,v)=sinθcoshvsinucosθsinhvcosuz(u,v)=vsinθ+ucosθ for (u,v)(π,π]×(,), with deformation parameter π<θπ, where:

  • θ=π corresponds to a right-handed helicoid,
  • θ=±π/2 corresponds to a catenoid, and
  • θ=0 corresponds to a left-handed helicoid.

References

Template:Reflist

Further reading

Template:Minimal surfaces

de:Minimalfläche#Das Katenoid