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Helicoid transformation: Adjusted anomation caption to point out that it's transforming between left- and right-handed helicoids. Swapped halves of parameterization to make similar parts line up better. (was a + b // -a + b; is now b + a // b - a)
 
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{{Short description|Surface of revolution of a catenary}}
[[Image:Catenoid.svg|thumb|right|alt=three-dimensional diagram of a catenoid|A catenoid]]
[[Image:Catenoid.svg|thumb|right|alt=three-dimensional diagram of a catenoid|A catenoid]]
[[Image:Catenoid.gif|thumb|right|alt=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]]
[[Image:Catenoid.gif|thumb|right|alt=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]]


A '''catenoid''' is a type of surface in [[topology]], arising by rotating a [[catenary]] curve about an axis.<ref>{{cite book|last1=Dierkes|first1=Ulrich|last2=Hildebrandt|first2=Stefan|last3=Sauvigny|first3=Friedrich|title=Minimal Surfaces|date=2010|publisher=Springer Science & Business Media|isbn=9783642116988|page=141|url=https://books.google.com/books?id=9YhBOg6vO-EC&pg=PA141|language=en}}</ref> It is a [[minimal surface]], meaning that it occupies the least area when bounded by a closed space.<ref name=Gullberg>{{cite book|last1=Gullberg|first1=Jan|title=Mathematics: From the Birth of Numbers|date=1997|publisher=W. W. Norton & Company|isbn=9780393040029|page=538|url=https://books.google.com/books?id=E09fBi9StpQC&pg=PA538|language=en}}</ref> It was formally described in 1744 by the mathematician [[Leonhard Euler]].
In [[geometry]], a '''catenoid''' is a type of [[Surface (mathematics)|surface]], arising by rotating a [[catenary]] curve about an axis (a [[surface of revolution]]).<ref>{{cite book|last1=Dierkes|first1=Ulrich|last2=Hildebrandt|first2=Stefan|last3=Sauvigny|first3=Friedrich|title=Minimal Surfaces|date=2010|publisher=[[Springer Science & Business Media]]|isbn=9783642116988|page=141|url=https://books.google.com/books?id=9YhBOg6vO-EC&pg=PA141|language=en}}</ref> It is a [[minimal surface]], meaning that it occupies the least area when bounded by a closed space.<ref name=Gullberg>{{cite book|last1=Gullberg|first1=Jan|title=Mathematics: From the Birth of Numbers|date=1997|publisher=[[W. W. Norton & Company]]|isbn=9780393040029|page=[https://archive.org/details/mathematicsfromb1997gull/page/538 538]|url=https://archive.org/details/mathematicsfromb1997gull|url-access=registration|language=en}}</ref> 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.<ref name=Gullberg/> 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.
[[Soap film]] attached to twin circular rings will take the shape of a catenoid.<ref name=Gullberg/> 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 dome shape of Inuit [[igloo]]s can be derived from rotation of a catenary about its central axis.
The catenoid was the first non-trivial minimal [[surface (topology)|surface]] in 3-dimensional Euclidean space to be discovered apart from the [[plane (geometry)|plane]]. The catenoid is obtained by rotating a catenary about its [[Directrix (conic section)|directrix]].<ref name=Gullberg/> It was found and proved to be minimal by [[Leonhard Euler]] in 1744.<ref>{{cite book|last1=Helveticae|first1=Euler, Leonhard |editor= Carathëodory Constantin |title=Methodus inveniendi lineas curvas: maximi minimive proprietate gaudentes sive solutio problematis isoperimetrici latissimo sensu accepti |date=1952 |orig-year=reprint of 1744 edition |publisher=Springer Science & Business Media |isbn=3-76431-424-9 |language=Latin |url=https://books.google.com/books?id=zNDdVFZalSAC}}</ref><ref name=Colding06>{{cite journal|last1=Colding|first1=T. H.|last2=Minicozzi|first2=W. P.|title=Shapes of embedded minimal surfaces|journal=Proceedings of the National Academy of Sciences|date=17 July 2006|volume=103|issue=30|pages=11106–11111|doi=10.1073/pnas.0510379103|pmc=1544050|pmid=16847265|bibcode=2006PNAS..10311106C|doi-access=free}}</ref>


Early work on the subject was published also by [[Jean Baptiste Meusnier]].<ref name=salvert>{{cite book|url=https://archive.org/details/mmoiresurlathor00salvgoog|format=PDF|last1=Meusnier|first1=J. B|title=Mémoire sur la courbure des surfaces|trans-title=Memory on the curvature of surfaces.|date=1881|publisher=F. Hayez, Imprimeur De L'Acdemie Royale De Belgique|location=Bruxelles|language=French|isbn=9781147341744|pages=477–510}}</ref><ref name=Colding06/>{{rp|11106}} There are only two [[minimal surfaces of revolution]] ([[surfaces of revolution]] which are also minimal surfaces): the [[plane (geometry)|plane]] and the catenoid.<ref>{{cite web|title=Catenoid|url=http://mathworld.wolfram.com/Catenoid.html|website=Wolfram MathWorld|accessdate=15 January 2017|language=en}}</ref>
==Geometry==
The catenoid was the first non-trivial minimal [[surface (topology)|surface]] in 3-dimensional Euclidean space to be discovered apart from the [[plane (geometry)|plane]]. The catenoid is obtained by rotating a catenary about its [[Directrix (conic section)|directrix]].<ref name=Gullberg/> It was found and proved to be minimal by [[Leonhard Euler]] in 1744.<ref>{{cite book|last1=Helveticae|first1=Euler, Leonhard |editor= Carathëodory Constantin |title=Methodus inveniendi lineas curvas: maximi minimive proprietate gaudentes sive solutio problematis isoperimetrici latissimo sensu accepti |date=1952 |orig-year=reprint of 1744 edition |publisher=Springer Science & Business Media |isbn=3-76431-424-9 |language=Latin |url=https://books.google.com/books/about/Methodus_inveniendi_lineas_curvas_maximi.html?id=zNDdVFZalSAC}}</ref>{{primary source inline|date=January 2017}}

Early work on the subject was published also by [[Jean Baptiste Meusnier]].<ref name=salvert>{{cite book|url=https://ia801406.us.archive.org/9/items/mmoiresurlathor00salvgoog/mmoiresurlathor00salvgoog.pdf|format=PDF|last1=Meusnier|first1=J. B|title=Mémoire sur la courbure des surfaces|trans-title=Memory on the curvature of surfaces.|date=1881|publisher=F. Hayez, Imprimeur De L'Acdemie Royale De Belgique|location=Bruxelles|language=French|isbn=9781147341744|pages=477–510}}</ref>{{primary source inline|date=January 2017}} There are only two [[minimal surfaces of revolution]] ([[surfaces of revolution]] which are also minimal surfaces): the [[plane (geometry)|plane]] and the catenoid.<ref>{{cite web|title=Catenoid|url=http://mathworld.wolfram.com/Catenoid.html|website=Wolfram MathWorld|accessdate=15 January 2017|language=en}}</ref>


The catenoid may be defined by the following parametric equations:
The catenoid may be defined by the following parametric equations:
<math display=block>\begin{align}

:<math>x=c \cosh \frac{v}{c} \cos u</math>
x &= c \cosh \frac{v}{c} \cos u \\
y &= c \cosh \frac{v}{c} \sin u \\

z &= v
:<math>y=c \cosh \frac{v}{c} \sin u</math>
\end{align}</math>

where <math>u \in [-\pi, \pi)</math> and <math>v \in \mathbb{R}</math> and <math>c</math> is a non-zero real constant.
:<math>z=v</math>

:where <math>u \in [-\pi, \pi)</math> and <math>v \in \mathbb{R}</math> and <math>c</math> is a non-zero real constant.


In cylindrical coordinates:
In cylindrical coordinates:
<math display=block>\rho =c \cosh \frac{z}{c},</math>
where <math>c</math> is a real constant.


A physical model of a catenoid can be formed by dipping two [[circle|circular]] rings into a soap solution and slowly drawing the circles apart.
:<math>\rho =c \cosh \frac{z}{c}</math>


The catenoid may be also defined approximately by the [[stretched grid method]] as a facet 3D model.
:where <math>c</math> 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 ==
== Helicoid transformation ==


[[Image:helicatenoid.gif|thumb|right|256px|alt=Continuous animation showing a helicoid deforming into a catenoid and back to a helicoid|Deformation of a [[helicoid]] into a catenoid]]
[[Image:helicatenoid.gif|thumb|right|256px|alt=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 function|continuous]] and [[Isometry|isometric]] deformation of a catenoid to a portion of the [[helicoid]] such that every member of the deformation family is [[Minimal surface|minimal]] (having a [[mean curvature]] of zero). A [[Parametric equation|parametrization]] of such a deformation is given by the system
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 function|continuous]] and [[Isometry|isometric]] deformation of a catenoid to a portion of the [[helicoid]] such that every member of the deformation family is [[Minimal surface|minimal]] (having a [[mean curvature]] of zero). A [[Parametric equation|parametrization]] of such a deformation is given by the system
<math display=block>\begin{align}
x(u,v) &= \sin \theta \,\cosh v \,\cos u + \cos \theta \,\sinh v \,\sin u \\
y(u,v) &= \sin \theta \,\cosh v \,\sin u - \cos \theta \,\sinh v \,\cos u \\
z(u,v) &= v \sin \theta + u \cos \theta
\end{align}</math>
for <math>(u,v) \in (-\pi, \pi] \times (-\infty, \infty)</math>, with deformation parameter <math>-\pi < \theta \le \pi</math>, where:
* <math>\theta = \pi</math> corresponds to a right-handed helicoid,
* <math>\theta = \pm \pi / 2</math> corresponds to a catenoid, and
* <math>\theta = 0</math> corresponds to a left-handed helicoid.


== References ==
:<math>x(u,v) = \cos \theta \,\sinh v \,\sin u + \sin \theta \,\cosh v \,\cos u</math>

:<math>y(u,v) = -\cos \theta \,\sinh v \,\cos u + \sin \theta \,\cosh v \,\sin u</math>

:<math>z(u,v) = u \cos \theta + v \sin \theta \,</math>

:for <math>(u,v) \in (-\pi, \pi] \times (-\infty, \infty)</math>, with deformation parameter <math>-\pi < \theta \le \pi</math>,

where
<math>\theta = \pi</math> corresponds to a right-handed helicoid,
<math>\theta = \pm \pi / 2</math> corresponds to a catenoid, and
<math>\theta = 0</math> corresponds to a left-handed helicoid.

== Architecture ==
{{further|Igloo#Engineering}}
[[File:Igloo spirale.svg|thumb|right|alt=cutaway diagram showing snow blocks in an igloo placed in an ascending spiral|spiral sequence of snow blocks in [[igloo]] construction]]

The [[Inuit]] learned to pattern the structure of their [[igloo]]s, or snow houses, after a shape with a catenary arch cross-section, which offers an optimal balance between height and diameter, avoiding the risk of collapsing under the weight of compacted snow.<ref name="Handy">{{cite journal|last1=Handy|first1=Richard L.|title=The Igloo and the Natural Bridge as Ultimate Structures|journal=Arctic|date=Dec 1973|volume=26|issue=4|pages=276–281|url=http://pubs.aina.ucalgary.ca/arctic/Arctic26-4-276.pdf|publisher=Arctic Institute of North America|format=PDF|doi=10.14430/arctic2926|quote=The Eskimo snow igloo is not a hemisphere as frequently depicted, but a catenoid of revolution with an optimum height-to-diameter ratio. This shape eliminates ring tension and shell moments and therefore prevents failure by caving or bulging.}}</ref> This differs from what is normally called a catenoid in that the catenary is rotated about its central axis, forming a surface with the topology of a bowl rather than that of a cylinder.

==References==
{{reflist}}
{{reflist}}


==Further reading==
== Further reading ==
* {{cite book |last1=Krivoshapko |first1=Sergey |last2=Ivanov |first2=V. N. |title=Encyclopedia of Analytical Surfaces |date=2015 |publisher=Springer |isbn=9783319117737 |chapter=Minimal Surfaces |chapter-url=https://books.google.com/books?id=cXTdBgAAQBAJ&pg=PA427 |language=en}}
* {{cite book |last1=Krivoshapko |first1=Sergey |last2=Ivanov |first2=V. N. |title=Encyclopedia of Analytical Surfaces |date=2015 |publisher=Springer |isbn=9783319117737 |chapter=Minimal Surfaces |chapter-url=https://books.google.com/books?id=cXTdBgAAQBAJ&pg=PA427 |language=en}}


==External links==
== External links ==
* {{springer|title=Catenoid|id=p/c020800}}
* {{springer|title=Catenoid|id=p/c020800}}
* [http://www.princeton.edu/~rvdb/WebGL/catenoid.html Catenoid - WebGL model]
* [http://www.princeton.edu/~rvdb/WebGL/catenoid.html Catenoid WebGL model]
* [http://posner.library.cmu.edu/Posner/books/book.cgi?call=517.4_E88M_1744 Euler's text describing the catenoid] at Carnegie Mellon University
* [http://posner.library.cmu.edu/Posner/books/book.cgi?call=517.4_E88M_1744 Euler's text describing the catenoid] at Carnegie Mellon University
* [https://www.youtube.com/watch?v=31Om4VrSzb8 Calculating the surface area of a Catenoid]
* [https://mathworld.wolfram.com/MinimalSurfaceofRevolution.html Minimal Surface of Revolution]


{{Minimal surfaces}}
{{Minimal surfaces}}


[[Category:Geometry]]
[[Category:Minimal surfaces]]
[[Category:Minimal surfaces]]


[[de:Minimalfläche#Die Katenoiden]]
[[de:Minimalfläche#Das Katenoid]]

Latest revision as of 07:43, 28 November 2024

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

[edit]

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]: 11106  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: where and and is a non-zero real constant.

In cylindrical coordinates: where 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

[edit]
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 for , with deformation parameter , where:

  • corresponds to a right-handed helicoid,
  • corresponds to a catenoid, and
  • corresponds to a left-handed helicoid.

References

[edit]
  1. ^ Dierkes, Ulrich; Hildebrandt, Stefan; Sauvigny, Friedrich (2010). Minimal Surfaces. Springer Science & Business Media. p. 141. ISBN 9783642116988.
  2. ^ a b c Gullberg, Jan (1997). Mathematics: From the Birth of Numbers. W. W. Norton & Company. p. 538. ISBN 9780393040029.
  3. ^ Helveticae, Euler, Leonhard (1952) [reprint of 1744 edition]. Carathëodory Constantin (ed.). Methodus inveniendi lineas curvas: maximi minimive proprietate gaudentes sive solutio problematis isoperimetrici latissimo sensu accepti (in Latin). Springer Science & Business Media. ISBN 3-76431-424-9.{{cite book}}: CS1 maint: multiple names: authors list (link)
  4. ^ a b Colding, T. H.; Minicozzi, W. P. (17 July 2006). "Shapes of embedded minimal surfaces". Proceedings of the National Academy of Sciences. 103 (30): 11106–11111. Bibcode:2006PNAS..10311106C. doi:10.1073/pnas.0510379103. PMC 1544050. PMID 16847265.
  5. ^ Meusnier, J. B (1881). Mémoire sur la courbure des surfaces [Memory on the curvature of surfaces.] (PDF) (in French). Bruxelles: F. Hayez, Imprimeur De L'Acdemie Royale De Belgique. pp. 477–510. ISBN 9781147341744.
  6. ^ "Catenoid". Wolfram MathWorld. Retrieved 15 January 2017.

Further reading

[edit]
[edit]