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Lu  \equiv  \sum _ {i, j= 1 } ^ { n }  
 
Lu  \equiv  \sum _ {i, j= 1 } ^ { n }  
 
a  ^ {ij} ( x) u _ {x _ {i}  x _ {j} } +
 
a  ^ {ij} ( x) u _ {x _ {i}  x _ {j} } +
\sum _ { j= } 1 ^ { n }  b  ^ {j} ( x) u _ {x _ {j}  } + b
+
\sum _ { j=1 } ^ { n }  b  ^ {j} ( x) u _ {x _ {j}  } + b
 
( x) u  =  f( x),
 
( x) u  =  f( x),
 
$$
 
$$
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$$  
 
$$  
 
\| u \| _ {C _ {1+ \alpha }  ( \Omega ) }  =  \| u \| _ {C _  \alpha  (
 
\| u \| _ {C _ {1+ \alpha }  ( \Omega ) }  =  \| u \| _ {C _  \alpha  (
\Omega ) } + \sum _ { i= } 1 ^ { n }  \| u _ {x _ {i}  } \| _ {C _  \alpha  ( \Omega ) } ,
+
\Omega ) } + \sum _ { i=1 } ^ { n }  \| u _ {x _ {i}  } \| _ {C _  \alpha  ( \Omega ) } ,
 
$$
 
$$
  
 
$$  
 
$$  
 
\| u \| _ {C _ {2+ \alpha }  ( \Omega ) }  =  \| u \| _ {C _ {1+ \alpha }  
 
\| u \| _ {C _ {2+ \alpha }  ( \Omega ) }  =  \| u \| _ {C _ {1+ \alpha }  
( \Omega ) } + \sum _ { i,j= } 1 ^ { n }  \| u _ {x _ {i}  x _ {j} } \| _ {C _  \alpha  ( \Omega ) } .
+
( \Omega ) } + \sum _ { i,j=1 } ^ { n }  \| u _ {x _ {i}  x _ {j} } \| _ {C _  \alpha  ( \Omega ) } .
 
$$
 
$$
  
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$$
 
$$
  
for the Laplace operator  $  \Delta = \sum _ {i=} 1 ^ {n} \partial  ^ {2} / \partial  x _ {i}  ^ {2} $.
+
for the Laplace operator  $  \Delta = \sum _ {i=1}  ^ {n} \partial  ^ {2} / \partial  x _ {i}  ^ {2} $.
  
 
5) Without loss of generality one may assume that  ,  
 
5) Without loss of generality one may assume that    \phi ( x) \equiv 0 ,  

Latest revision as of 16:50, 4 January 2021


A method for solving boundary value problems for linear uniformly-elliptic equations of the second order, based on a priori estimates and the continuation method (see also Continuation method (to a parametrized family)).

Schauder's method of finding a solution to the Dirichlet problem for a linear uniformly-elliptic equation

\tag{1 } Lu \equiv \sum _ {i, j= 1 } ^ { n } a ^ {ij} ( x) u _ {x _ {i} x _ {j} } + \sum _ { j=1 } ^ { n } b ^ {j} ( x) u _ {x _ {j} } + b ( x) u = f( x),

given in a bounded domain \Omega of a Euclidean space of points x= ( x _ {1} \dots x _ {n} ) and with a coefficient b( x) \leq 0 , can be described in the following way.

1) The spaces C _ \alpha ( \Omega ) , C _ {1+ \alpha } ( \Omega ) and C _ {2+ \alpha } ( \Omega ) are introduced as sets of functions u = u( x) with finite norms

\| u \| _ {C _ \alpha ( \Omega ) } = \sup _ {x \in \Omega } | u( x) | + \sup _ {x,y } \frac{u( x)- u( y) }{| x- y | ^ \alpha } ,\ \ 0 < \alpha < 1,

\| u \| _ {C _ {1+ \alpha } ( \Omega ) } = \| u \| _ {C _ \alpha ( \Omega ) } + \sum _ { i=1 } ^ { n } \| u _ {x _ {i} } \| _ {C _ \alpha ( \Omega ) } ,

\| u \| _ {C _ {2+ \alpha } ( \Omega ) } = \| u \| _ {C _ {1+ \alpha } ( \Omega ) } + \sum _ { i,j=1 } ^ { n } \| u _ {x _ {i} x _ {j} } \| _ {C _ \alpha ( \Omega ) } .

2) It is assumed that the boundary \sigma of the domain \Omega is of class C _ {2 + \alpha } , i.e. each element \sigma _ {x} of the ( n- 1) - dimensional surface \sigma can be mapped on a part of the plane by a coordinate transformation y= y( x) with a positive Jacobian, moreover, u \in C _ {2 + \alpha } ( \sigma _ {x} ) .

3) It is proved that if the coefficients of (1) belong to the space C _ \alpha ( \Omega ) and if the function u \in C _ {2+ \alpha } ( \Omega ) , then the a priori estimate

\tag{2 } \| u \| _ {C _ {2+ \alpha } ( \Omega ) } \leq C \left [ \| Lu \| _ {C _ \alpha ( \Omega ) } + \| u \| _ {C _ {2+ \alpha } ( \Omega ) } + \| u \| _ {C _ {0} ( \Omega ) } \right ]

is true up to the boundary, where the constant C depends only on \Omega , on the ellipticity constant m \leq a ^ {ij} ( x) \xi _ {i} \xi _ {j} / | \xi | ^ {2} , \xi \neq 0 , and on the norms of the coefficients of the operator L , and where

\| u \| _ {C _ {0} ( \Omega ) } = \sup _ {x \in \Omega } | u( x) | .

4) It is assumed that one knows how to prove the existence of a solution u \in C _ {2+ \alpha } to the Dirichlet problem

\left . u \right | _ \sigma = \left . \phi \right | _ \sigma ,\ \ \phi \in C _ {2+ \alpha } ( \Omega ) ,

for the Laplace operator \Delta = \sum _ {i=1} ^ {n} \partial ^ {2} / \partial x _ {i} ^ {2} .

5) Without loss of generality one may assume that \phi ( x) \equiv 0 , and then apply the continuation method, the essence of which is the following:

5 _ {1} . The operator L is imbedded in a one-parameter family of operators

L _ {t} u = tLu + ( 1- t) \Delta u ,\ \ 0 \leq t \leq 1,\ \ L _ {0} = \Delta .

5 _ {2} . Basing oneself essentially on the a priori estimate (2), it can be established that the set T of those values of t \in [ 0, 1] for which the Dirichlet problem L _ {t} u = f( x) , u \mid _ \sigma = 0 , has a solution u \in C _ {2+ \alpha } ( \Omega ) for all f \in C _ \alpha ( \Omega ) , is at the same time open and closed, and thus coincides with the unit interval [ 0, 1] .

6) It is proved that if D is a bounded domain contained in \Omega together with its closure, then for any function u \in C _ {2+ \alpha } ( D) and any compact subdomain \omega \subset D the interior a priori estimate

\tag{3 } \| u \| _ {C _ {2+ \alpha } ( \omega ) } \leq C \left [ \| Lu \| _ {C _ \alpha ( D) } + \| u \| _ {C _ {0} ( D) } \right ]

holds.

7) Approximating uniformly the functions \phi and f by functions from C _ {2+ \alpha } and applying the estimate (3), one proves the existence of a solution to the Dirichlet problem for any continuous boundary function and for a wide class of domains with non-smooth boundaries, e.g. for domains that can be represented as the union of sequences of domains \Omega _ {1} \subset \Omega _ {2} \subset \dots , with boundaries of the same smoothness as \sigma .

Estimates 2 and 3 where first obtained by J. Schauder (see [1], [2]) and go under his name. Schauder's estimates and his method have been generalized to equations and systems of higher order. The a priori estimates, both interior and up to the boundary, corresponding to it are sometimes called Schauder-type estimates. The method of a priori estimates is a further generalization of Schauder's method.

References

[1] J. Schauder, "Ueber lineare elliptische Differentialgleichungen zweiter Ordnung" Math. Z. , 38 : 2 (1934) pp. 257–282
[2] J. Schauder, "Numerische Abschätzungen in elliptischen linearen Differentialgleichungen" Studia Math. , 5 (1935) pp. 34–42
[3] L. Bers, F. John, M. Schechter, "Partial differential equations" , Interscience (1964)
[4] R. Courant, D. Hilbert, "Methods of mathematical physics. Partial differential equations" , 2 , Interscience (1965) (Translated from German)
[5] A.V. Bitsadze, "Some classes of partial differential equations" , Gordon & Breach (1988) (Translated from Russian)
[6] Yu.M. [Yu.M. Berezanskii] Berezanskiy, "Expansion in eigenfunctions of selfadjoint operators" , Amer. Math. Soc. (1968) (Translated from Russian)
[7] O.A. Ladyzhenskaya, N.N. Ural'tseva, "Linear and quasilinear elliptic equations" , Acad. Press (1968) (Translated from Russian)

Comments

Schauder-type estimates for parabolic equations were obtained for the first time in [a1] (see also [a2] for a detailed description).

References

[a1] C. Ciliberto, "Formule di maggiorazione e teoremi di esistenza per le soluzioni delle equazioni paraboliche in due variabili" Ricerche Mat. , 3 (1954) pp. 40–75
[a2] A. Friedman, "Partial differential equations of parabolic type" , Prentice-Hall (1964)
[a3] D. Gilbarg, N.S. Trudinger, "Elliptic partial differential equations of second order" , Springer (1977)
How to Cite This Entry:
Schauder method. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Schauder_method&oldid=48617
This article was adapted from an original article by A.M. Nakhushev (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098. See original article