Difference between revisions of "Fundamental solution"
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''of a linear partial differential equation'' | ''of a linear partial differential equation'' | ||
− | A solution of a partial differential equation | + | A solution of a partial differential equation $ Lu ( x) = 0 $, |
+ | $ x \in \mathbf R ^ {n} $, | ||
+ | with coefficients of class $ C ^ \infty $, | ||
+ | in the form of a function $ I ( x, y) $ | ||
+ | that satisfies, for fixed $ y \in \mathbf R ^ {n} $, | ||
+ | the equation | ||
+ | |||
+ | $$ | ||
+ | L I ( x, y) = \delta ( x - y),\ \ | ||
+ | x \neq y, | ||
+ | $$ | ||
+ | |||
+ | which is interpreted in the sense of the theory of generalized functions, where $ \delta $ | ||
+ | is the [[Delta-function|delta-function]]. There is a fundamental solution for every partial differential equation with constant coefficients, and also for arbitrary elliptic equations. For example, for the elliptic equation | ||
− | + | $$ | |
+ | \sum _ {i, j = 1 } ^ { n } | ||
+ | a _ {ij} | ||
+ | \frac{\partial ^ {2} u }{\partial x _ {i} \partial x _ {j} } | ||
+ | = 0 | ||
+ | $$ | ||
− | + | with constant coefficients $ a _ {ij} $ | |
+ | forming a positive-definite matrix $ a $, | ||
+ | a fundamental solution is provided by the function | ||
− | + | $$ | |
+ | I ( x, y) = \ | ||
+ | \left \{ | ||
+ | \begin{array}{l} | ||
+ | \left [ \sum _ {i, j = 1 } ^ { n } | ||
+ | A _ {ij} ( x _ {i} - y _ {i} ) ( x _ {j} - y _ {j} ) | ||
+ | \right ] ^ {( 2 - n)/2 } ,\ n > 2 , | ||
+ | \\ | ||
− | + | \mathop{\rm log} \left [ \sum _ {i, j = 1 } ^ { n } | |
+ | A _ {ij} ( x _ {i} - y _ {i} ) ( x _ {j} - y _ {j} ) \right ] ,\ n = 2 , | ||
+ | \end{array} | ||
− | + | $$ | |
− | where | + | where $ A _ {ij} $ |
+ | is the cofactor of $ a _ {ij} $ | ||
+ | in the matrix $ a $. | ||
Fundamental solutions are widely used in the study of boundary value problems for elliptic equations. | Fundamental solutions are widely used in the study of boundary value problems for elliptic equations. | ||
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====References==== | ====References==== | ||
<table><TR><TD valign="top">[1]</TD> <TD valign="top"> V.S. Vladimirov, "Generalized functions in mathematical physics" , MIR (1979) (Translated from Russian)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> L. Bers, F. John, M. Schechter, "Partial differential equations" , Interscience (1964)</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> F. John, "Plane waves and spherical means: applied to partial differential equations" , Interscience (1955)</TD></TR></table> | <table><TR><TD valign="top">[1]</TD> <TD valign="top"> V.S. Vladimirov, "Generalized functions in mathematical physics" , MIR (1979) (Translated from Russian)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> L. Bers, F. John, M. Schechter, "Partial differential equations" , Interscience (1964)</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> F. John, "Plane waves and spherical means: applied to partial differential equations" , Interscience (1955)</TD></TR></table> | ||
− | |||
− | |||
====Comments==== | ====Comments==== |
Revision as of 19:40, 5 June 2020
of a linear partial differential equation
A solution of a partial differential equation $ Lu ( x) = 0 $, $ x \in \mathbf R ^ {n} $, with coefficients of class $ C ^ \infty $, in the form of a function $ I ( x, y) $ that satisfies, for fixed $ y \in \mathbf R ^ {n} $, the equation
$$ L I ( x, y) = \delta ( x - y),\ \ x \neq y, $$
which is interpreted in the sense of the theory of generalized functions, where $ \delta $ is the delta-function. There is a fundamental solution for every partial differential equation with constant coefficients, and also for arbitrary elliptic equations. For example, for the elliptic equation
$$ \sum _ {i, j = 1 } ^ { n } a _ {ij} \frac{\partial ^ {2} u }{\partial x _ {i} \partial x _ {j} } = 0 $$
with constant coefficients $ a _ {ij} $ forming a positive-definite matrix $ a $, a fundamental solution is provided by the function
$$ I ( x, y) = \ \left \{ \begin{array}{l} \left [ \sum _ {i, j = 1 } ^ { n } A _ {ij} ( x _ {i} - y _ {i} ) ( x _ {j} - y _ {j} ) \right ] ^ {( 2 - n)/2 } ,\ n > 2 , \\ \mathop{\rm log} \left [ \sum _ {i, j = 1 } ^ { n } A _ {ij} ( x _ {i} - y _ {i} ) ( x _ {j} - y _ {j} ) \right ] ,\ n = 2 , \end{array} $$
where $ A _ {ij} $ is the cofactor of $ a _ {ij} $ in the matrix $ a $.
Fundamental solutions are widely used in the study of boundary value problems for elliptic equations.
References
[1] | V.S. Vladimirov, "Generalized functions in mathematical physics" , MIR (1979) (Translated from Russian) |
[2] | L. Bers, F. John, M. Schechter, "Partial differential equations" , Interscience (1964) |
[3] | F. John, "Plane waves and spherical means: applied to partial differential equations" , Interscience (1955) |
Comments
Fundamental solutions are also used in the study of Cauchy problems (cf. Cauchy problem) for hyperbolic and parabolic equations. The name "elementary solution of a linear partial differential equationelementary solution" is also used.
See also Green function.
References
[a1] | A. Friedman, "Partial differential equations of parabolic type" , Prentice-Hall (1964) |
[a2] | O.A. Ladyzhenskaya, N.N. Ural'tseva, "Linear and quasilinear elliptic equations" , Acad. Press (1968) (Translated from Russian) |
[a3] | O.A. Ladyzhenskaya, V.A. Solonnikov, N.N. Ural'tseva, "Linear and quasilinear parabolic equations" , Amer. Math. Soc. (1968) (Translated from Russian) |
[a4] | L. Schwartz, "Théorie des distributions" , 1–2 , Hermann (1957–1959) |
[a5] | I.M. Gel'fand, G.E. Shilov, "Generalized functions" , Acad. Press (1964) (Translated from Russian) |
Fundamental solution. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Fundamental_solution&oldid=11510