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	<title>Rec. 2020 - Revision history</title>
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		<title>en&gt;GrandDrake: /* Implementations */ Added link</title>
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		<summary type="html">&lt;p&gt;&lt;span class=&quot;autocomment&quot;&gt;Implementations: &lt;/span&gt; Added link&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;[[File:Bulle caténoïde.png|thumb|240px|Stretching a soap film between two parallel circular wire loops generates a [[catenoid]]al minimal surface of revolution]]&lt;br /&gt;
In [[mathematics]], a &amp;#039;&amp;#039;&amp;#039;minimal surface of revolution&amp;#039;&amp;#039;&amp;#039; or &amp;#039;&amp;#039;&amp;#039;minimum surface of revolution&amp;#039;&amp;#039;&amp;#039; is a [[surface of revolution]] defined from two [[point (geometry)|points]] in a [[half-plane]], whose boundary is the axis of revolution of the surface. It is generated by a [[curve]] that lies in the half-plane and connects the two points; among all the surfaces that can be generated in this way, it is the one that [[mathematical optimization|minimizes]] the [[surface area]].&amp;lt;ref name=&amp;quot;Mathworld: Minimal Surface of Revolution&amp;quot;&amp;gt;{{cite web | url=http://mathworld.wolfram.com/MinimalSurfaceofRevolution.html | title=Minimal Surface of Revolution | last=Weisstein | first=Eric W. | authorlink=Eric W. Weisstein | work=[[Mathworld]] | publisher=[[Wolfram Research]] | accessdate=2012-08-29}}&amp;lt;/ref&amp;gt; A basic problem in the [[calculus of variations]] is finding the curve between two points that produces this minimal surface of revolution.&amp;lt;ref name=&amp;quot;Mathworld: Minimal Surface of Revolution&amp;quot;/&amp;gt;&lt;br /&gt;
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==Relation to minimal surfaces==&lt;br /&gt;
A minimal surface of revolution is a subtype of [[minimal surface]].&amp;lt;ref name=&amp;quot;Mathworld: Minimal Surface of Revolution&amp;quot;/&amp;gt; A minimal surface is defined not as a surface of minimal area, but as a surface with a [[mean curvature]] of 0.&amp;lt;ref name=&amp;quot;Mathworld: Minimal Surface&amp;quot;&amp;gt;{{cite web | url=http://mathworld.wolfram.com/MinimalSurface.html | title=Minimal Surface | last=Weisstein | first=Eric W. | authorlink=Eric W. Weisstein | work=[[Mathworld]] | publisher=[[Wolfram Research]] | accessdate=2012-08-29}}&amp;lt;/ref&amp;gt; Since a mean curvature of 0 is a [[necessary condition]] of a surface of minimal area, all minimal surfaces of revolution are minimal surfaces, but not all minimal surfaces are minimal surfaces of revolution. As a point forms a [[circle]] when [[rotation around a fixed axis|rotated about an axis]], finding the minimal surface of revolution is equivalent to finding the minimal surface passing through two circular [[wireframe model|wireframes]].&amp;lt;ref name=&amp;quot;Mathworld: Minimal Surface of Revolution&amp;quot;/&amp;gt; A physical realization of a minimal surface of revolution is [[soap film]] stretched between two parallel circular [[wire]]s: the soap film naturally takes on the shape with least surface area.&amp;lt;ref name=&amp;quot;Peter J. Olver&amp;quot;&amp;gt;{{cite book | title=Applied Mathematics Lecture Notes | last=Olver | first=Peter J. | chapter=Chapter 21: The Calculus of Variations | year=2012 | url=http://www.math.umn.edu/~olver/am_/cvz.pdf | format=PDF | accessdate=2012-08-29}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;When Least Is Best-Soap and Solution&amp;quot;&amp;gt;&lt;br /&gt;
{{cite book | title=When Least Is Best: How Mathematicians Discovered Many Clever Ways to Make Things as Small (or as Large) as Possible | last=Nahin | first=Paul J. | publisher=[[Princeton University Press]] | year=2011 | page=265-6 | quote=So what happens to the soap film after it breaks [...]? This discontinuous behavior is called the &amp;#039;&amp;#039;Goldschmidt solution&amp;#039;&amp;#039;, after the German mathematician [[C. W. B. Goldschmidt]] (1807-51) who discovered it (on paper) in 1831.}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
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==Catenoid solution==&lt;br /&gt;
[[File:Catenoid.svg|thumb|A [[catenoid]]]]&lt;br /&gt;
If the half-plane containing the two points and the axis of revolution is given [[Cartesian coordinate]]s, making the axis of revolution into the &amp;#039;&amp;#039;x&amp;#039;&amp;#039;-axis of the coordinate system, then the curve connecting the points may be interpreted as the [[graph of a function]]. If the Cartesian coordinates of the two given points are &amp;lt;math&amp;gt;(x_1,y_1)&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;(x_2,y_2)&amp;lt;/math&amp;gt;, then the area of the surface generated by a [[continuous function]] &amp;lt;math&amp;gt;f&amp;lt;/math&amp;gt; may be expressed mathematically as&lt;br /&gt;
:&amp;lt;math&amp;gt;2\pi\int_{x_1}^{x_2} f(x) \sqrt{1+f&amp;#039;(x)^2} dx&amp;lt;/math&amp;gt;&lt;br /&gt;
and the problem of finding the minimal surface of revolution becomes one of finding the function that minimizes this integral, subject to the [[boundary conditions]] that &amp;lt;math&amp;gt;f(x_1)=y_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;f(x_2)=y_2&amp;lt;/math&amp;gt;.&amp;lt;ref name=&amp;quot;sagan&amp;quot;/&amp;gt; In this case, the optimal curve will necessarily be a [[catenary]].&amp;lt;ref name=&amp;quot;Mathworld: Minimal Surface of Revolution&amp;quot;/&amp;gt;&amp;lt;ref name=&amp;quot;sagan&amp;quot;/&amp;gt; The axis of revolution is the directrix of the catenary, and the minimal surface of revolution will thus be a [[catenoid]].&amp;lt;ref name=&amp;quot;Mathworld: Minimal Surface of Revolution&amp;quot;/&amp;gt;&amp;lt;ref name=&amp;quot;Colding and Minicozzi&amp;quot;&amp;gt;{{cite book | title=A Course in Minimal Surfaces | series=Graduate Studies in Mathematics | last1=Colding | first1=Tobias Holck | authorlink1=Tobias Colding | last2=Minicozzi II | first2=William P. | chapter=Chapter 1: The Beginning of the Theory | publisher=[[American Mathematical Society]] | year=2011 | url=http://www.ams.org/bookstore/pspdf/gsm-121-prev.pdf | format=PDF | accessdate=2012-08-29}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Meeks and Perez&amp;quot;&amp;gt;{{cite book | title=A Survey on Classical Minimal Surface Theory | series=University Lectures Series | volume=60 | last1=Meeks III | first1=William H. | last2=Pérez | first2=Joaquín | chapter=Chapter 2.5: Some interesting examples of complete minimal surfaces. | publisher=[[American Mathematical Society]] | year=2012 | url=http://www.ugr.es/~jperez/papers/monograph-book2.pdf | format=PDF | accessdate=2012-08-29}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Goldschmidt solution==&lt;br /&gt;
Solutions based on discontinuous functions may also be defined. In particular, for some placements of the two points the optimal solution is generated by a discontinuous function that is nonzero at the two points and zero everywhere else. This function leads to a surface of revolution consisting of two circular disks, one for each point, connected by a degenerate line segment along the axis of revolution. This is known as a &amp;#039;&amp;#039;&amp;#039;Goldschmidt solution&amp;#039;&amp;#039;&amp;#039;&amp;lt;ref name=&amp;quot;sagan&amp;quot;&amp;gt;{{citation|contribution=2.6 The problem of minimal surfaces of revolution|title=Introduction to the Calculus of Variations|first=Hans|last=Sagan|publisher=Courier Dover Publications|year=1992|isbn=9780486673660|url=http://books.google.com/books?id=abhS8PgpBskC&amp;amp;pg=PA62|pages=62–66}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Mathworld: Goldschmidt Solution&amp;quot;&amp;gt;{{cite web | url=http://mathworld.wolfram.com/GoldschmidtSolution.html | title=Goldschmidt Solution | last=Weisstein | first=Eric W. | authorlink=Eric W. Weisstein | work=[[Mathworld]] | publisher=[[Wolfram Research]] | accessdate=2012-08-29}}&amp;lt;/ref&amp;gt; after [[German people|German]] mathematician [[Carl Wolfgang Benjamin Goldschmidt]],&amp;lt;ref name=&amp;quot;When Least Is Best-Soap and Solution&amp;quot;/&amp;gt; who announced his discovery of it in his 1831 paper &amp;quot;Determinatio superficiei minimae rotatione curvae data duo puncta jungentis circa datum axem ortae&amp;quot; (&amp;quot;Determination of the surface-minimal rotation curve given two joined points about a given axis of origin&amp;quot;).&amp;lt;ref&amp;gt;{{cite web | url=http://books.google.com/books/about/Determinatio_superficiei_minimae_rotatio.html?id=bPs-AAAAYAAJ | title=Bibliographic Information: Determinatio superficiei minimae rotatione curvae data duo puncta jungentis circa datum axem ortae | publisher=[[Google Books]] | accessdate=2012-08-27}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
To continue the physical analogy of soap film given above, these Goldschmidt solutions can be visualized as instances in which the soap film breaks as the circular wires are stretched apart.&amp;lt;ref name=&amp;quot;When Least Is Best-Soap and Solution&amp;quot;/&amp;gt; However, in a physical soap film, the connecting line segment would not be present. Additionally, if a soap film is stretched in this way, there is a range of distances within which the catenoid solution is still feasible but has greater area than the Goldschmidt solution, so the soap film may stretch into a configuration in which the area is a [[local minimum]] but not a global minimum. For distances greater than this range, the catenary that defines the catenoid crosses the &amp;#039;&amp;#039;x&amp;#039;&amp;#039;-axis and leads to a self-intersecting surface, so only the Goldschmidt solution is feasible.&amp;lt;ref&amp;gt;{{citation|title=The Science of Soap Films and Soap Bubbles|first=Cyril|last=Isenberg|authorlink=Cyril Isenberg|publisher=Courier Dover Publications|year=1992|isbn=9780486269603|page=165|url=http://books.google.com/books?id=PdsVME_LXTYC&amp;amp;pg=PA165}}.&amp;lt;/ref&amp;gt;&lt;br /&gt;
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==References==&lt;br /&gt;
&lt;br /&gt;
{{reflist}}&lt;br /&gt;
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[[Category:Minimal surfaces]]&lt;/div&gt;</summary>
		<author><name>en&gt;GrandDrake</name></author>
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