Plateau's problem: Difference between revisions

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  | doi=10.1007/BF01404309| bibcode = 1969InMat...7..243B
  | doi=10.1007/BF01404309| bibcode = 1969InMat...7..243B
  | s2cid = 59816096
  | s2cid = 59816096
  }}</ref> To solve the extended problem in certain special cases, the [[Caccioppoli set#De Giorgi definition|theory of perimeters]] ([[Ennio De Giorgi|De Giorgi]]) for codimension 1 and the theory of [[rectifiable current]]s ([[Herbert Federer|Federer]] and Fleming) for higher codimension have been developed. The theory guarantees existence of codimension 1 solutions that are smooth away from a closed set of [[Hausdorff dimension]] <math>n-8</math>. In the case of higher codimension [[Frederick J. Almgren, Jr.|Almgren]] proved existence of solutions with [[singular set]] of dimension at most <math>k-2</math> in his [[Almgren regularity theorem|regularity theorem]]. S. X. Chang, a
  }}</ref> To solve the extended problem in certain special cases, the [[Caccioppoli set#De Giorgi definition|theory of perimeters]] ([[Ennio De Giorgi|De Giorgi]]) for codimension 1 and the theory of rectifiable currents ([[Herbert Federer|Federer]] and Fleming) for higher codimension have been developed. The theory guarantees existence of codimension 1 solutions that are smooth away from a closed set of [[Hausdorff dimension]] <math>n-8</math>. In the case of higher codimension [[Frederick J. Almgren, Jr.|Almgren]] proved existence of solutions with [[singular set]] of dimension at most <math>k-2</math> in his Almgren regularity theorem|regularity theorem. S. X. Chang, a
student of Almgren, built upon Almgren’s work to show that the singularities of 2-dimensional area
student of Almgren, built upon Almgren’s work to show that the singularities of 2-dimensional area
minimizing integral currents (in arbitrary codimension) form a finite discrete set.<ref>
minimizing integral currents (in arbitrary codimension) form a finite discrete set.<ref>
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  | year = 2016}}</ref>
  | year = 2016}}</ref>


The axiomatic approach of [[Jenny Harrison]] and [[Harrison Pugh]]<ref>{{citation
The axiomatic approach of [[Jenny Harrison]] and Harrison Pugh<ref>{{citation
| last1 = Harrison | first1 = Jenny
| last1 = Harrison | first1 = Jenny
| last2 = Pugh | first2 = Harrison
| last2 = Pugh | first2 = Harrison
| title = General Methods of Elliptic Minimization
| title = General Methods of Elliptic Minimization
| journal = [[Calculus of Variations and Partial Differential Equations]]
| journal = Calculus of Variations and Partial Differential Equations
| volume = 56
| volume = 56
| year = 2017
| year = 2017
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| arxiv = 1603.04492
| arxiv = 1603.04492
| s2cid = 119704344
| s2cid = 119704344
}}</ref> treats a wide variety of special cases. In particular, they solve the anisotropic Plateau problem in arbitrary dimension and codimension for any collection of rectifiable sets satisfying a combination of general homological, cohomological or homotopical spanning conditions. A different proof of Harrison-Pugh's results were obtained by [[Camillo De Lellis]], Francesco Ghiraldin and [[Francesco Maggi]].<ref>{{citation
}}</ref> treats a wide variety of special cases. In particular, they solve the anisotropic Plateau problem in arbitrary dimension and codimension for any collection of rectifiable sets satisfying a combination of general homological, cohomological or homotopical spanning conditions. A different proof of Harrison-Pugh's results were obtained by [[Camillo De Lellis]], Francesco Ghiraldin and Francesco Maggi.<ref>{{citation
  | last1 = De Lellis | first1 = Camillo
  | last1 = De Lellis | first1 = Camillo
  | last2 = Ghiraldin | first2 = Francesco
  | last2 = Ghiraldin | first2 = Francesco
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==Physical applications==
==Physical applications==
Physical soap films are more accurately modeled by the <math>(M, 0, \Delta)</math>-minimal sets of [[Frederick Almgren]], but the lack of a compactness theorem makes it difficult to prove the existence of an area minimizer. In this context, a persistent open question has been the existence of a least-area soap film. [[Ernst Robert Reifenberg]] solved such a "universal Plateau's problem" for boundaries which are homeomorphic to single embedded spheres.
Physical soap films are more accurately modeled by the <math>(M, 0, \Delta)</math>-minimal sets of [[Frederick Almgren]], but the lack of a compactness theorem makes it difficult to prove the existence of an area minimizer. In this context, a persistent open question has been the existence of a least-area soap film. Ernst Robert Reifenberg solved such a "universal Plateau's problem" for boundaries which are homeomorphic to single embedded spheres.


==See also==
==See also==

Latest revision as of 16:56, 9 December 2025

Template:Short description

File:Bulle caténoïde.png
A soap bubble in the shape of a catenoid

Script error: No such module "sidebar". In mathematics, Plateau's problem is to show the existence of a minimal surface with a given boundary, a problem raised by Joseph-Louis Lagrange in 1760. However, it is named after Joseph Plateau who experimented with soap films. The problem is considered part of the calculus of variations. The existence and regularity problems are part of geometric measure theory.

History

Various specialized forms of the problem were solved, but it was only in 1930 that general solutions were found in the context of mappings (immersions) independently by Jesse Douglas and Tibor Radó. Their methods were quite different; Radó's work built on the previous work of René Garnier and held only for rectifiable simple closed curves, whereas Douglas used completely new ideas with his result holding for an arbitrary simple closed curve. Both relied on setting up minimization problems; Douglas minimized the now-named Douglas integral while Radó minimized the "energy". Douglas went on to be awarded the Fields Medal in 1936 for his efforts.

In higher dimensions

The extension of the problem to higher dimensions (that is, for k-dimensional surfaces in n-dimensional space) turns out to be much more difficult to study. Moreover, while the solutions to the original problem are always regular, it turns out that the solutions to the extended problem may have singularities if kn2. In the hypersurface case where k=n1, singularities occur only for n8. An example of such singular solution of the Plateau problem is the Simons cone, a cone over S3×S3 in 8 that was first described by Jim Simons and was shown to be an area minimizer by Bombieri, De Giorgi and Giusti.[1] To solve the extended problem in certain special cases, the theory of perimeters (De Giorgi) for codimension 1 and the theory of rectifiable currents (Federer and Fleming) for higher codimension have been developed. The theory guarantees existence of codimension 1 solutions that are smooth away from a closed set of Hausdorff dimension n8. In the case of higher codimension Almgren proved existence of solutions with singular set of dimension at most k2 in his Almgren regularity theorem|regularity theorem. S. X. Chang, a student of Almgren, built upon Almgren’s work to show that the singularities of 2-dimensional area minimizing integral currents (in arbitrary codimension) form a finite discrete set.[2][3]

The axiomatic approach of Jenny Harrison and Harrison Pugh[4] treats a wide variety of special cases. In particular, they solve the anisotropic Plateau problem in arbitrary dimension and codimension for any collection of rectifiable sets satisfying a combination of general homological, cohomological or homotopical spanning conditions. A different proof of Harrison-Pugh's results were obtained by Camillo De Lellis, Francesco Ghiraldin and Francesco Maggi.[5]

Physical applications

Physical soap films are more accurately modeled by the (M,0,Δ)-minimal sets of Frederick Almgren, but the lack of a compactness theorem makes it difficult to prove the existence of an area minimizer. In this context, a persistent open question has been the existence of a least-area soap film. Ernst Robert Reifenberg solved such a "universal Plateau's problem" for boundaries which are homeomorphic to single embedded spheres.

See also

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References

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This article incorporates material from Plateau's Problem on PlanetMath, which is licensed under the Creative Commons Attribution/Share-Alike License.