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In [[mathematics]], a '''Dirichlet problem''' is the problem of finding a [[function (mathematics)|function]] which solves a specified [[partial differential equation]] (PDE) in the interior of a given region that takes prescribed values on the boundary of the region.
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The Dirichlet problem can be solved for many PDEs, although originally it was posed for [[Laplace's equation]]. In that case the problem can be stated as follows:
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:Given a function ''f'' that has values everywhere on the boundary of a region in '''R'''<sup>''n''</sup>, is there a unique [[continuous function]] ''u'' twice continuously differentiable in the interior and continuous on the boundary, such that ''u'' is [[harmonic function|harmonic]] in the interior and ''u''&nbsp;=&nbsp;''f'' on the boundary?
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This requirement is called the [[Dirichlet boundary condition]].  The main issue is to prove the existence of a solution; uniqueness can be proved using the [[maximum principle]].
'''MathML'''
:<math forcemathmode="mathml">E=mc^2</math>


==History==
<!--'''PNG''' (currently default in production)
The '''Dirichlet problem''' is named after [[Johann Peter Gustav Lejeune Dirichlet|Lejeune Dirichlet]], who proposed a solution by a variational method which became known as [[Dirichlet's principle]]. The existence of a unique solution is very plausible by the 'physical argument': any charge distribution on the boundary should, by the laws of [[electrostatics]], determine an [[electrical potential]] as solution.
:<math forcemathmode="png">E=mc^2</math>


However, [[Weierstrass]] found a flaw in Dirichlet's argument, and a rigorous proof of existence was found only in 1900 by [[David Hilbert|Hilbert]]. It turns out that the existence of a solution depends delicately on the smoothness of the boundary and the prescribed data.
'''source'''
:<math forcemathmode="source">E=mc^2</math> -->


== General solution ==
<span style="color: red">Follow this [https://en.wikipedia.org/wiki/Special:Preferences#mw-prefsection-rendering link] to change your Math rendering settings.</span> You can also add a [https://en.wikipedia.org/wiki/Special:Preferences#mw-prefsection-rendering-skin Custom CSS] to force the MathML/SVG rendering or select different font families. See [https://www.mediawiki.org/wiki/Extension:Math#CSS_for_the_MathML_with_SVG_fallback_mode these examples].
For a domain <math>D</math> having a sufficiently smooth boundary <math>\partial D</math>, the general solution to the Dirichlet problem is given by 


:<math>u(x)=\int_{\partial D} \nu(s) \frac{\partial G(x,s)}{\partial n} ds</math>
==Demos==


where <math>G(x,y)</math> is the [[Green's function]] for the partial differential equation, and
Here are some [https://commons.wikimedia.org/w/index.php?title=Special:ListFiles/Frederic.wang demos]:


:<math>\frac{\partial G(x,s)}{\partial n} = \widehat{n} \cdot \nabla_s G (x,s) = \sum_i n_i \frac{\partial G(x,s)}{\partial s_i}</math>


is the derivative of the Green's function along the inward-pointing unit normal vector <math>\widehat{n}</math>. The integration is performed on the boundary, with [[Measure (mathematics)|measure]] <math>ds</math>. The function <math>\nu(s)</math> is given by the unique solution to the [[Fredholm integral equation]] of the second kind,
* accessibility:
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** From our testing, ChromeVox and JAWS are not able to read the formulas generated by the MathML mode.


:<math>f(x) = -\frac{\nu(x)}{2} + \int_{\partial D} \nu(s) \frac{\partial G(x,s)}{\partial n} ds.</math>
==Test pages ==


The Green's function to be used in the above integral is one which vanishes on the boundary:
To test the '''MathML''', '''PNG''', and '''source''' rendering modes, please go to one of the following test pages:
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:<math>G(x,s)=0</math>
*[[Inputtypes|Inputtypes (private Wikis only)]]
 
*[[Url2Image|Url2Image (private Wikis only)]]
for <math>s\in \partial D</math> and <math>x\in D</math>. Such a Green's function is usually a sum of the free-field Green's function and a harmonic solution to the differential equation.
==Bug reporting==
 
If you find any bugs, please report them at [https://bugzilla.wikimedia.org/enter_bug.cgi?product=MediaWiki%20extensions&component=Math&version=master&short_desc=Math-preview%20rendering%20problem Bugzilla], or write an email to math_bugs (at) ckurs (dot) de .
===Existence===
The Dirichlet problem for harmonic functions always has a solution, and that solution is unique, when the boundary is sufficiently smooth and <math>f(s)</math> is continuous. More precisely, it has a solution when
 
:<math>\partial D \in C^{(1,\alpha)}</math>
 
for <math>0<\alpha</math>, where <math>C^{(1,\alpha)}</math> denotes the [[Hölder condition]].
 
== Example: the unit disk in two dimensions ==
In some simple cases the Dirichlet problem can be solved explicitly.  For example, the solution to the Dirichlet problem for the unit disk in '''R'''<sup>2</sup> is given by the [[Poisson integral formula]].
 
If <math>f</math> is a continuous function on the boundary <math>\partial D</math> of the open unit disk <math>D</math>, then the solution to the Dirichlet problem is <math>u(z)</math> given by
 
:<math>u(z) = \begin{cases} \frac{1}{2\pi}\int_0^{2\pi} f(e^{i\psi})
\frac {1-\vert z \vert ^2}{\vert 1-ze^{-i\psi}\vert ^2} d \psi & \mbox{if }z \in D \\
f(z) & \mbox{if }z \in \partial D. \end{cases}</math>
 
The solution <math>u</math> is continuous on the closed unit disk <math>\bar{D}</math> and harmonic on <math>D.</math>
 
The integrand is known as the [[Poisson kernel]]; this solution follows from the Green's function in two dimensions:
 
:<math>G(z,x) = -\frac{1}{2\pi} \log \vert z-x\vert + \gamma(z,x)</math>
 
where <math>\gamma(z,x)</math> is harmonic
 
:<math>\Delta_x \gamma(z,x)=0</math>
 
and chosen such that <math>G(z,x)=0</math> for <math>x\in \partial D</math>.
==Methods of solution==
For bounded domains, the Dirichlet problem can be solved using the [[Perron method]], which relies on the [[maximum principle]] for [[subharmonic function]]s. This approach is described in many text books.<ref> See for example:
*{{harvnb|John|1982}}
*{{harvnb|Bers|John|Schechter|1979}}
*{{harvnb|Greene|Krantz|2006}}
</ref> It is not well-suited to describing smoothness of solutions when the boundary is smooth. Another classical [[Hilbert space]] approach through [[Sobolev space]]s does yield such information.<ref> See for example:
*{{harvnb|Bers|John|Schechter|1979}}
*{{harvnb|Chazarain|Piriou|1982}}
*{{harvnb|Taylor|2011}}
</ref> The solution of the Dirichlet problem using [[Sobolev spaces for planar domains]] can be used to prove the smooth version of the [[Riemann mapping theorem]]. {{harvtxt|Bell|1992}} has outlined a different approach for establishing the smooth Riemann mapping theorem, based on the [[reproducing kernel]]s of Szegő and Bergman, and in turn used it to solve the Dirichlet problem. The classical methods of [[potential theory]] allow the Dirichlet problem to be solved directly in terms of [[integral operator]]s, for which the standard theory of [[compact operator|compact]] and [[Fredholm operator]]s is applicable. The same methods work equally for the [[Neumann problem]].
<ref>See:
*{{harvnb|Folland|1995}}
*{{harvnb|Bers|John|Schechter|1979}}</ref>
 
==Generalizations==
Dirichlet problems are typical of [[elliptic partial differential equation]]s, and [[potential theory]], and the [[Laplace equation]] in particular. Other examples include the [[biharmonic equation]] and related equations in [[elasticity theory]].
 
They are one of several types of classes of PDE problems defined by the information given at the boundary, including [[Neumann problem]]s and [[Cauchy problem]]s.
 
==Notes==
{{reflist|2}}
 
==References==
* {{springer|author=A. Yanushauskas|id=d/d032910|title=Dirichlet problem}}
* S. G. Krantz, ''The Dirichlet Problem.''  §7.3.3 in ''Handbook of Complex Variables''. Boston, MA: Birkhäuser, p. 93, 1999. ISBN 0-8176-4011-8.
* S. Axler, P. Gorkin, K. Voss, ''[http://www.ams.org/mcom/2004-73-246/S0025-5718-03-01574-6/home.html The Dirichlet problem on quadratic surfaces]'' Mathematics of Computation '''73''' (2004), 637-651.
*{{Citation | last1=Gilbarg | first1=David | last2=Trudinger | first2=Neil S. | author2-link=Neil Trudinger | title=Elliptic partial differential equations of second order | publisher=[[Springer-Verlag]] | location=Berlin, New York | edition=2nd | isbn=978-3-540-41160-4 | year=2001}}
*Gérard, Patrick; [[Eric Leichtnam|Leichtnam, Éric]]: Ergodic properties of eigenfunctions for the Dirichlet problem. Duke Math. J. 71 (1993), no. 2, 559-607.
*{{citation|last=John|first= Fritz|title=Partial differential equations|edition=4th|series= Applied Mathematical Sciences|volume= 1|publisher= Springer-Verlag|year= 1982|id= ISBN 0-387-90609-6}}
*{{citation|last=Bers|first=Lipman|last2=John|first2=Fritz|last3= Schechter|first3= Martin|title=Partial differential equations, with supplements by Lars Gȧrding and A. N. Milgram|series= Lectures in Applied Mathematics|volume= 3A|publisher= American Mathematical Society|year=1979|id=ISBN 0-8218-0049-3}}
*{{citation|title=Lectures on Elliptic Boundary Value Problems|first=Shmuel|last= Agmon|authorlink=Shmuel Agmon|year=2010|publisher=American Mathematical Society|id=ISBN 0-8218-4910-7}}
* {{citation|first=Elias M.|last= Stein|authorlink=Elias Stein|year=1970|title=Singular Integrals and Differentiability Properties of Functions|publisher=Princeton University Press}}
*{{citation|last=Greene|first= Robert E.|last2= Krantz|first2= Steven G.|title= Function theory of one complex variable|edition=3rd|series= Graduate Studies in Mathematics|volume= 40|publisher= American Mathematical Society|year= 2006|id= ISBN 0-8218-3962-4}}
*{{citation| last=Taylor|first= Michael E.|title= Partial differential equations I. Basic theory|edition=2nd |series= Applied Mathematical Sciences|volume= 115|publisher=Springer|year=2011|id= ISBN 978-1-4419-70}}
*{{citation|last=Zimmer|first= Robert J.|title= Essential results of functional analysis|series= Chicago Lectures in Mathematics|publisher= University of Chicago Press|year= 1990|id= ISBN 0-226-98337-4}}
*{{citation|last=Folland|first= Gerald B.|title= Introduction to partial differential equations|edition=2nd|publisher=Princeton University Press|year=1995|id= ISBN 0-691-04361-2}}
*{{citation|title=Introduction to the Theory of Linear Partial Differential Equations|volume=14|series= Studies in Mathematics and Its Applications|first=Jacques|last= Chazarain|first2= Alain|last2= Piriou|publisher=Elsevier|year= 1982|id=ISBN 0444864520}}
*{{citation|last=Bell|first=Steven R.|title= The Cauchy transform, potential theory, and conformal mapping|series= Studies in Advanced Mathematics|publisher= CRC Press|year= 1992|id=ISBN 0-8493-8270-X}}
*{{citation|title=Foundations of Differentiable Manifolds and Lie Groups|series=Graduate Texts in Mathematics|volume= 94|year=1983|
first=Frank W.|last= Warner|id=ISBN 0387908943|publisher=Springer}}
*{{citation|title=Principles of Algebraic Geometry|first=Phillip |last=Griffiths|first2= Joseph|last2= Harris|publisher= Wiley Interscience| year=1994|id=ISBN  0471050598}}
*{{citation|last=Courant|first= R.|title=Dirichlet's Principle, Conformal Mapping, and Minimal Surfaces|
publisher=Interscience|year= 1950}}
*{{citation|last=Schiffer|first= M.|last2=Hawley|first2= N. S.|title=Connections and conformal mapping|journal=
Acta Math.|volume= 107|year= 1962|pages= 175–274}}
 
== External links ==
* {{MathWorld | urlname=DirichletProblem | title=Dirichlet Problem}}
* [http://math.fullerton.edu/mathews/c2003/DirichletProblemMod.html Dirichlet Problem Module by John H. Mathews]
 
[[Category:Potential theory]]
[[Category:Partial differential equations]]
[[Category:Fourier analysis]]
[[Category:Mathematical problems]]
 
[[ca:Problema de Dirichlet]]
[[es:Problema de Dirichlet]]
[[fr:Problème de Dirichlet]]
[[ko:디리클레 문제]]
[[ja:ディリクレ問題]]
[[pms:Problema ëd Dirichlet]]
[[pl:Problem Dirichleta]]
[[pt:Problema de Dirichlet]]
[[ru:Задача Дирихле]]
[[tr:Dirichlet problemi]]
[[zh:狄利克雷问题]]

Latest revision as of 22:52, 15 September 2019

This is a preview for the new MathML rendering mode (with SVG fallback), which is availble in production for registered users.

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E=mc2


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