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Difference between revisions of "Strong solution"

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''of a differential equation''
 
''of a differential equation''
  
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$$Lu\equiv\sum_{|\alpha|\leq m}a_\alpha(x)D^\alpha u=f\label{*}\tag{*}$$
  
 
''in a domain D''
 
''in a domain D''
  
A locally integrable function u that has locally integrable generalized derivatives of all orders \leq m (cf. [[Generalized derivative|Generalized derivative]]), and satisfies \ref{*} almost-everywhere in D.
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A locally integrable function u that has locally integrable generalized derivatives of all orders \leq m (cf. [[Generalized derivative|Generalized derivative]]), and satisfies \eqref{*} almost-everywhere in D.
  
The notion of a  "strong solution"  can also be introduced as follows. A function u is called a strong solution of \ref{*} if there are sequences of smooth (for example, C^\infty) functions \{u_n\}, \{f_n\} such that u_n\to u, f_n\to f and Lu_n=f_n for each n, where the convergence is taken in L_1(K) for any compact set K\subseteq D. In these definitions, L_1 can be replaced by the class L_p of functions whose p-th powers are locally integrable. The class most often used is L_2.
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The notion of a  "strong solution"  can also be introduced as follows. A function u is called a strong solution of \eqref{*} if there are sequences of smooth (for example, C^\infty) functions \{u_n\}, \{f_n\} such that u_n\to u, f_n\to f and Lu_n=f_n for each n, where the convergence is taken in L_1(K) for any compact set K\subseteq D. In these definitions, L_1 can be replaced by the class L_p of functions whose p-th powers are locally integrable. The class most often used is L_2.
  
In the case of an elliptic equation \ref{*} both notions of a strong solution coincide.
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In the case of an elliptic equation \eqref{*} both notions of a strong solution coincide.
  
  

Latest revision as of 15:58, 14 February 2020

of a differential equation

Lu\equiv\sum_{|\alpha|\leq m}a_\alpha(x)D^\alpha u=f\label{*}\tag{*}

in a domain D

A locally integrable function u that has locally integrable generalized derivatives of all orders \leq m (cf. Generalized derivative), and satisfies \eqref{*} almost-everywhere in D.

The notion of a "strong solution" can also be introduced as follows. A function u is called a strong solution of \eqref{*} if there are sequences of smooth (for example, C^\infty) functions \{u_n\}, \{f_n\} such that u_n\to u, f_n\to f and Lu_n=f_n for each n, where the convergence is taken in L_1(K) for any compact set K\subseteq D. In these definitions, L_1 can be replaced by the class L_p of functions whose p-th powers are locally integrable. The class most often used is L_2.

In the case of an elliptic equation \eqref{*} both notions of a strong solution coincide.


Comments

References

[a1] J. Chazarain, A. Piriou, "Introduction à la théorie des équations aux dérivées partielles linéaires" , Gauthier-Villars (1981) pp. 223 MR0598467 Zbl 0446.35001
How to Cite This Entry:
Strong solution. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Strong_solution&oldid=32910
This article was adapted from an original article by A.P. Soldatov (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098. See original article