Minimal Smooth Surface Spanned by Contour
Theorem
Let $\map z {x, y}: \R^2 \to \R$ be a real-valued function.
Let $\Gamma$ be a closed contour in $3$-dimensional Euclidean space.
Then the smooth surface of least area spanned by the contour $\Gamma$ has to satisfy the following Euler's equation:
- $r \paren {1 + q^2} - 2 s p q + t \paren {1 + p^2} = 0$
where:
\(\ds p\) | \(=\) | \(\ds z_x\) | ||||||||||||
\(\ds q\) | \(=\) | \(\ds z_y\) | ||||||||||||
\(\ds r\) | \(=\) | \(\ds z_{xx}\) | ||||||||||||
\(\ds s\) | \(=\) | \(\ds z_{xy}\) | ||||||||||||
\(\ds t\) | \(=\) | \(\ds z_{yy}\) |
with subscript denoting respective partial derivatives.
In other words, its mean curvature has to vanish.
Proof
The surface area for a smooth surface embedded in $3$-dimensional Euclidean space is given by:
- $\ds A \sqbrk z = \iint_\Gamma \sqrt {1 + z_x^2 + z_y^2} \rd x \rd y$
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It follows that:
\(\ds \dfrac \d {\d x} \frac \partial {\partial z_x} \sqrt {1 + z_x^2 + z_y^2}\) | \(=\) | \(\ds \dfrac \d {\d x} \frac {z_x} {\sqrt {1 + z_x^2 + z_y^2} }\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \frac {z_{xx} + z_y^2 z_{xx} - z_x z_y z_{xy} } {\paren {1 + z_x^2 + z_y^2}^{\frac 3 2} }\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \frac {r \paren {1 + q^2} - p q s } {\paren {1 + p^2 + q^2}^{\frac 3 2} }\) |
\(\ds \dfrac \d {\d y} \frac \partial {\partial z_y} \sqrt {1 + z_x^2 + z_y^2}\) | \(=\) | \(\ds \dfrac \d {\d y} \frac {z_y} {\sqrt {1 + z_x^2 + z_y^2} }\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \frac {z_{yy} + z_x^2 z_{yy} - z_x z_y z_{xy} } {\paren {1 + z_x^2 + z_y^2}^{\frac 3 2} }\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \frac {t \paren {1 + p^2} - p q s } {\paren {1 + p^2 + q^2}^{\frac 3 2} }\) |
By Euler's equation:
- $\dfrac {r \paren {1 + q^2} - 2 s p q + t \paren {1 + p^2} } {\paren {1 + p^2 + q^2}^{\frac 3 2} } = 0$
Due to the smoothness of the surface, $1 + p^2 + q^2$ is bounded.
Hence, the following equation is sufficient:
- $r \paren {1 + q^2} - 2 s p q + t \paren {1 + p^2} = 0$
Introduce the following change of variables:
\(\ds E\) | \(=\) | \(\ds 1 + p^2\) | ||||||||||||
\(\ds F\) | \(=\) | \(\ds p q\) | ||||||||||||
\(\ds G\) | \(=\) | \(\ds 1 + q^2\) | ||||||||||||
\(\ds e\) | \(=\) | \(\ds \dfrac r {\sqrt {1 + p^2 + q ^2} }\) | ||||||||||||
\(\ds f\) | \(=\) | \(\ds \dfrac s {\sqrt {1 + p^2 + q^2} }\) | ||||||||||||
\(\ds g\) | \(=\) | \(\ds \dfrac t {\sqrt {1 + p^2 + q^2} }\) |
Then Euler's equation can be rewritten as:
- $\dfrac {E g - 2 F f + G e} {2 \paren {E G - F^2} } = 0$
By definition, mean curvature is:
- $M = \dfrac {E g - 2 F f + G e} {2 \paren {E G - F^2} }$
Hence:
- $M = 0$
$\blacksquare$
Sources
- 1963: I.M. Gelfand and S.V. Fomin: Calculus of Variations ... (previous) ... (next): $\S 1.5$: The Case of Several Variables