Difference between revisions of "Poisson formula"
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The same as [[Poisson integral|Poisson integral]]. | The same as [[Poisson integral|Poisson integral]]. | ||
− | A formula giving an integral representation for the solution of the [[Cauchy problem|Cauchy problem]] for the [[Wave equation|wave equation]] in | + | A formula giving an integral representation for the solution of the [[Cauchy problem|Cauchy problem]] for the [[Wave equation|wave equation]] in $ \mathbf R ^ {3} $: |
+ | |||
+ | $$ | ||
− | + | \frac{\partial ^ {2} u }{\partial t ^ {2} } | |
− | + | - a ^ {2} \Delta u = 0 ,\ \ | |
+ | t > 0 ,\ M = ( x , y , z ) , | ||
+ | $$ | ||
− | < | + | $$ |
+ | - \infty < x , y , z < \infty , | ||
+ | $$ | ||
+ | |||
+ | $$ | ||
+ | u ( M , 0 ) = \phi ( M) ,\ | ||
+ | \frac{\partial u ( M , 0 ) }{\partial t } | ||
+ | = \psi ( M) . | ||
+ | $$ | ||
This solution has the form | This solution has the form | ||
− | + | $$ \tag{1 } | |
+ | u ( M , t ) = \ | ||
+ | |||
+ | \frac \partial {\partial t } | ||
+ | |||
+ | \{ t \Gamma _ {at} ( \phi ) \} + t \Gamma _ {at} ( \psi ) , | ||
+ | $$ | ||
where | where | ||
− | + | $$ | |
+ | \Gamma _ {at} ( \phi ) = \ | ||
+ | |||
+ | \frac{1}{4 \pi } | ||
+ | |||
+ | \int\limits _ {S _ {at} } \phi ( P) d \Omega | ||
+ | $$ | ||
− | is the mean value of the function | + | is the mean value of the function $ \phi $ |
+ | on the sphere $ S _ {at} $ | ||
+ | in the $ ( x , y , z ) $- | ||
+ | space of radius $ a t $ | ||
+ | and centre at the point $ M $, | ||
+ | and $ d \Omega $ | ||
+ | is the area element on the unit sphere. In the case of the inhomogeneous wave equation a third term is added to formula (1) (see ). | ||
From formula (1), by the method of descent (cf. [[Descent, method of|Descent, method of]]) formulas are obtained for solving the Cauchy problem in two- (Poisson's formula) and one- (d'Alembert formula) dimensional space (see ). See also [[Kirchhoff formula|Kirchhoff formula]]. | From formula (1), by the method of descent (cf. [[Descent, method of|Descent, method of]]) formulas are obtained for solving the Cauchy problem in two- (Poisson's formula) and one- (d'Alembert formula) dimensional space (see ). See also [[Kirchhoff formula|Kirchhoff formula]]. | ||
− | Sometimes the phrase "Poisson formula" is used for the integral representation of the solution to the Cauchy problem for the [[Heat equation|heat equation]] in the space | + | Sometimes the phrase "Poisson formula" is used for the integral representation of the solution to the Cauchy problem for the [[Heat equation|heat equation]] in the space $ \mathbf R ^ {3} $: |
+ | |||
+ | $$ | ||
− | + | \frac{\partial u }{\partial t } | |
+ | - a ^ {2} \Delta u = 0 ,\ \ | ||
+ | t > 0 ,\ M = ( x , y , z ) , | ||
+ | $$ | ||
− | + | $$ | |
+ | - \infty < x , y , z < \infty , | ||
+ | $$ | ||
− | + | $$ | |
+ | u ( M , 0 ) = \phi ( M) . | ||
+ | $$ | ||
This solution has the form | This solution has the form | ||
− | + | $$ \tag{2 } | |
+ | u ( M , t ) = \ | ||
+ | |||
+ | \frac{1}{( 2 \sqrt {\pi a ^ {2} t } ) ^ {3} } | ||
− | Formula (2) immediately generalizes to an | + | \int\limits _ {\mathbf R ^ {3} } |
+ | \phi ( P) e ^ {| M P | ^ {2} / 4 a ^ {2} t } d \sigma ( P) . | ||
+ | $$ | ||
+ | |||
+ | Formula (2) immediately generalizes to an $ n $- | ||
+ | dimensional space, $ n \geq 1 $. | ||
====References==== | ====References==== | ||
<table><TR><TD valign="top">[1]</TD> <TD valign="top"> S.D. Poisson, ''Mém. Acad. Sci. Paris'' , '''3''' (1818) pp. 121–176</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> A.N. Tikhonov, A.A. Samarskii, "Equations of mathematical physics" , Pergamon (1963) (Translated from Russian)</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> V.S. Vladimirov, "Equations of mathematical physics" , MIR (1984) (Translated from Russian)</TD></TR></table> | <table><TR><TD valign="top">[1]</TD> <TD valign="top"> S.D. Poisson, ''Mém. Acad. Sci. Paris'' , '''3''' (1818) pp. 121–176</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> A.N. Tikhonov, A.A. Samarskii, "Equations of mathematical physics" , Pergamon (1963) (Translated from Russian)</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> V.S. Vladimirov, "Equations of mathematical physics" , MIR (1984) (Translated from Russian)</TD></TR></table> | ||
− | |||
− | |||
====Comments==== | ====Comments==== | ||
− | |||
====References==== | ====References==== | ||
<table><TR><TD valign="top">[a1]</TD> <TD valign="top"> G.B. Whitham, "Linear and non-linear waves" , Wiley (Interscience) (1974) pp. 229ff</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> A.V. Bitsadze, "Equations of mathematical physics" , MIR (1980) pp. 179 (Translated from Russian)</TD></TR></table> | <table><TR><TD valign="top">[a1]</TD> <TD valign="top"> G.B. Whitham, "Linear and non-linear waves" , Wiley (Interscience) (1974) pp. 229ff</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> A.V. Bitsadze, "Equations of mathematical physics" , MIR (1980) pp. 179 (Translated from Russian)</TD></TR></table> |
Latest revision as of 08:06, 6 June 2020
The same as Poisson integral.
A formula giving an integral representation for the solution of the Cauchy problem for the wave equation in $ \mathbf R ^ {3} $:
$$ \frac{\partial ^ {2} u }{\partial t ^ {2} } - a ^ {2} \Delta u = 0 ,\ \ t > 0 ,\ M = ( x , y , z ) , $$
$$ - \infty < x , y , z < \infty , $$
$$ u ( M , 0 ) = \phi ( M) ,\ \frac{\partial u ( M , 0 ) }{\partial t } = \psi ( M) . $$
This solution has the form
$$ \tag{1 } u ( M , t ) = \ \frac \partial {\partial t } \{ t \Gamma _ {at} ( \phi ) \} + t \Gamma _ {at} ( \psi ) , $$
where
$$ \Gamma _ {at} ( \phi ) = \ \frac{1}{4 \pi } \int\limits _ {S _ {at} } \phi ( P) d \Omega $$
is the mean value of the function $ \phi $ on the sphere $ S _ {at} $ in the $ ( x , y , z ) $- space of radius $ a t $ and centre at the point $ M $, and $ d \Omega $ is the area element on the unit sphere. In the case of the inhomogeneous wave equation a third term is added to formula (1) (see ).
From formula (1), by the method of descent (cf. Descent, method of) formulas are obtained for solving the Cauchy problem in two- (Poisson's formula) and one- (d'Alembert formula) dimensional space (see ). See also Kirchhoff formula.
Sometimes the phrase "Poisson formula" is used for the integral representation of the solution to the Cauchy problem for the heat equation in the space $ \mathbf R ^ {3} $:
$$ \frac{\partial u }{\partial t } - a ^ {2} \Delta u = 0 ,\ \ t > 0 ,\ M = ( x , y , z ) , $$
$$ - \infty < x , y , z < \infty , $$
$$ u ( M , 0 ) = \phi ( M) . $$
This solution has the form
$$ \tag{2 } u ( M , t ) = \ \frac{1}{( 2 \sqrt {\pi a ^ {2} t } ) ^ {3} } \int\limits _ {\mathbf R ^ {3} } \phi ( P) e ^ {| M P | ^ {2} / 4 a ^ {2} t } d \sigma ( P) . $$
Formula (2) immediately generalizes to an $ n $- dimensional space, $ n \geq 1 $.
References
[1] | S.D. Poisson, Mém. Acad. Sci. Paris , 3 (1818) pp. 121–176 |
[2] | A.N. Tikhonov, A.A. Samarskii, "Equations of mathematical physics" , Pergamon (1963) (Translated from Russian) |
[3] | V.S. Vladimirov, "Equations of mathematical physics" , MIR (1984) (Translated from Russian) |
Comments
References
[a1] | G.B. Whitham, "Linear and non-linear waves" , Wiley (Interscience) (1974) pp. 229ff |
[a2] | A.V. Bitsadze, "Equations of mathematical physics" , MIR (1980) pp. 179 (Translated from Russian) |
Poisson formula. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Poisson_formula&oldid=14431