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Richmond surface

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Minimal surface in differential geometry
Richmond surface for m=2.

In differential geometry, a Richmond surface is a minimal surface first described by Herbert William Richmond in 1904. It is a family of surfaces with one planar end and one Enneper surface-like self-intersecting end.

It has Weierstrass–Enneper parameterization f ( z ) = 1 / z 2 , g ( z ) = z m {\displaystyle f(z)=1/z^{2},g(z)=z^{m}} . This allows a parametrization based on a complex parameter as

X ( z ) = [ ( 1 / 2 z ) z 2 m + 1 / ( 4 m + 2 ) ] Y ( z ) = [ ( i / 2 z ) + i z 2 m + 1 / ( 4 m + 2 ) ] Z ( z ) = [ z m / m ] {\displaystyle {\begin{aligned}X(z)&=\Re \\Y(z)&=\Re \\Z(z)&=\Re \end{aligned}}}

The associate family of the surface is just the surface rotated around the z-axis.

Taking m = 2 a real parametric expression becomes:

X ( u , v ) = ( 1 / 3 ) u 3 u v 2 + u u 2 + v 2 Y ( u , v ) = u 2 v + ( 1 / 3 ) v 3 v u 2 + v 2 Z ( u , v ) = 2 u {\displaystyle {\begin{aligned}X(u,v)&=(1/3)u^{3}-uv^{2}+{\frac {u}{u^{2}+v^{2}}}\\Y(u,v)&=-u^{2}v+(1/3)v^{3}-{\frac {v}{u^{2}+v^{2}}}\\Z(u,v)&=2u\end{aligned}}}

References

  1. Jesse Douglas, Tibor Radó, The Problem of Plateau: A Tribute to Jesse Douglas & Tibor Radó, World Scientific, 1992 (p. 239-240)
  2. John Oprea, The Mathematics of Soap Films: Explorations With Maple, American Mathematical Soc., 2000
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