← Iris
Catenoid

Surface properties

Surface Catenoid
Vertices 0
Faces 0
Mean curvature H = 0
Morph 0%

Catenoid

The surface of revolution of a catenary curve. The only minimal surface of revolution besides the plane. Two parallel rings dipped in soap produce this shape.

Click + drag to rotate the 3D view  ·  Use the morph slider to continuously deform between conjugate surfaces  ·  Adjust mesh resolution to see more or less detail
Resolution30
Morph (Catenoid ↔ Helicoid)0%
Scale1.0

About this lab

What are minimal surfaces?

A minimal surface is one where the mean curvature is zero at every point. Intuitively, this means the surface curves equally in opposite directions — saddle-shaped locally, never dome-shaped. Soap films naturally form minimal surfaces because surface tension acts to minimize area. Given a wire frame boundary, the soap film finds the least-area surface spanning that boundary — this is Plateau’s problem, posed by Joseph Plateau in 1873 and not rigorously solved until Jesse Douglas and Tibor Radó independently proved the existence of solutions in 1930–31. Douglas won one of the first Fields Medals for this work.

The catenoid-helicoid deformation

The catenoid and helicoid are conjugate minimal surfaces, related by the Weierstrass-Enneper parametrization. They can be continuously deformed into each other through a one-parameter family of minimal surfaces — every intermediate surface also has zero mean curvature. This is the “associated family” of a minimal surface, parametrized by the angle θ in the formula: X(θ) = Re(e^(iθ) · Φ) where Φ is the holomorphic null curve. At θ = 0 you get the catenoid; at θ = π/2, the helicoid.

The Enneper surface and beyond

The Enneper surface, discovered by Alfred Enneper in 1864, is the simplest minimal surface that self-intersects. Its parametrization is polynomial: x = u - u³/3 + uv², y = v - v³/3 + vu², z = u² - v². Despite looking exotic, it satisfies the same mean curvature condition as a flat plane. Scherk’s surface (1834) was the third minimal surface discovered, after the plane and catenoid. Its doubly-periodic saddle towers appear in the architecture of Frei Otto and in the microstructure of block copolymers.

Why minimal surfaces matter

Beyond soap films, minimal surfaces appear in materials science (grain boundaries in crystals), architecture (tensile structures), biology (cell membranes, lung alveoli), and general relativity (apparent horizons of black holes). The mathematics connects to complex analysis, differential geometry, and the calculus of variations. Every minimal surface can be locally described by holomorphic data — a deep connection between the geometry of least area and the algebra of complex numbers.