Difference between revisions of "Gellerstedt problem"
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A boundary value problem for a Chaplygin-type equation | A boundary value problem for a Chaplygin-type equation | ||
− | + | $$ | |
+ | K ( y) z _ {xx} + z _ {yy} = 0, | ||
+ | $$ | ||
− | in which the function | + | in which the function $ K( y) $ |
+ | increases, $ K( 0) = 0 $ | ||
+ | and $ yK ( y) > 0 $ | ||
+ | for $ y \neq 0 $. | ||
+ | The function $ z( x, y) $ | ||
+ | which is to be found is specified on the boundary. This boundary consists of a sufficiently-smooth contour and pieces of characteristics. This equation is elliptic in the half-plane $ y > 0 $, | ||
+ | parabolic on the line $ y = 0 $, | ||
+ | and hyperbolic for $ y < 0 $. | ||
+ | The half-plane of hyperbolicity is covered by two families of characteristics, which satisfy the equations $ y ^ \prime = {[ - K( y) ] } ^ {- 1/2 } $ | ||
+ | and $ y ^ \prime = {-[- K( y)] } ^ {- 1/2 } $. | ||
<img style="border:1px solid;" src="https://www.encyclopediaofmath.org/legacyimages/common_img/g043640a.gif" /> | <img style="border:1px solid;" src="https://www.encyclopediaofmath.org/legacyimages/common_img/g043640a.gif" /> | ||
Line 9: | Line 32: | ||
Figure: g043640a | Figure: g043640a | ||
− | The characteristics of one of these families merge with the characteristics of the other on the line | + | The characteristics of one of these families merge with the characteristics of the other on the line $ y = 0 $. |
− | Let | + | Let $ E $ |
+ | be a simply-connected domain with as boundary a sufficiently-smooth contour $ \Gamma $ | ||
+ | if $ y \geq 0 $ | ||
+ | or pieces $ \Gamma _ {1} $, | ||
+ | $ \Gamma _ {2} $, | ||
+ | $ \Gamma _ {3} $, | ||
+ | and $ \Gamma _ {4} $ | ||
+ | if $ y \leq 0 $, | ||
+ | $ \Gamma _ {1} $ | ||
+ | and $ \Gamma _ {3} $ | ||
+ | being the characteristics of one family, and $ \Gamma _ {2} $ | ||
+ | and $ \Gamma _ {4} $ | ||
+ | of the other (see Fig.). The theorem on the existence and the uniqueness of solutions of the following boundary value problems is valid in $ E $: | ||
+ | the function $ z( x, y) $ | ||
+ | is given on $ \Gamma + \Gamma _ {1} + \Gamma _ {4} $; | ||
+ | the function $ z( x, y) $ | ||
+ | is given on $ \Gamma + \Gamma _ {2} + \Gamma _ {3} $. | ||
− | These problems were first studied (for | + | These problems were first studied (for $ K( y) = \mathop{\rm sgn} y \cdot | y | ^ \alpha $, |
+ | $ \alpha > 0 $) | ||
+ | by S. Gellerstedt [[#References|[1]]] by methods developed by F. Tricomi [[#References|[2]]] for the [[Tricomi problem|Tricomi problem]], and represent a generalization of that problem. Gellerstedt's problem has important applications in gas dynamics with velocities around the velocity of sound. These and related problems were studied for certain multiply-connected domains and for linear equations containing lower-order terms [[#References|[3]]]. | ||
====References==== | ====References==== | ||
<table><TR><TD valign="top">[1]</TD> <TD valign="top"> S. Gellerstedt, "Quelques problèmes mixtes pour l'équation <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/g/g043/g043640/g04364032.png" />" ''Ark. Mat. Astr. Fysik'' , '''26A''' : 3 (1937) pp. 1–32</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> F.G. Tricomi, "Integral equations" , Interscience (1957)</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> M.M. Smirnov, "Equations of mixed type" , Amer. Math. Soc. (1978) (Translated from Russian)</TD></TR></table> | <table><TR><TD valign="top">[1]</TD> <TD valign="top"> S. Gellerstedt, "Quelques problèmes mixtes pour l'équation <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/g/g043/g043640/g04364032.png" />" ''Ark. Mat. Astr. Fysik'' , '''26A''' : 3 (1937) pp. 1–32</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> F.G. Tricomi, "Integral equations" , Interscience (1957)</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> M.M. Smirnov, "Equations of mixed type" , Amer. Math. Soc. (1978) (Translated from Russian)</TD></TR></table> | ||
− | |||
− | |||
====Comments==== | ====Comments==== | ||
− | |||
====References==== | ====References==== | ||
<table><TR><TD valign="top">[a1]</TD> <TD valign="top"> L. Bers, "Mathematical aspects of subsonic and transonic gas dynamics" , Wiley (1958)</TD></TR></table> | <table><TR><TD valign="top">[a1]</TD> <TD valign="top"> L. Bers, "Mathematical aspects of subsonic and transonic gas dynamics" , Wiley (1958)</TD></TR></table> |
Latest revision as of 19:41, 5 June 2020
A boundary value problem for a Chaplygin-type equation
$$ K ( y) z _ {xx} + z _ {yy} = 0, $$
in which the function $ K( y) $ increases, $ K( 0) = 0 $ and $ yK ( y) > 0 $ for $ y \neq 0 $. The function $ z( x, y) $ which is to be found is specified on the boundary. This boundary consists of a sufficiently-smooth contour and pieces of characteristics. This equation is elliptic in the half-plane $ y > 0 $, parabolic on the line $ y = 0 $, and hyperbolic for $ y < 0 $. The half-plane of hyperbolicity is covered by two families of characteristics, which satisfy the equations $ y ^ \prime = {[ - K( y) ] } ^ {- 1/2 } $ and $ y ^ \prime = {-[- K( y)] } ^ {- 1/2 } $.
Figure: g043640a
The characteristics of one of these families merge with the characteristics of the other on the line $ y = 0 $.
Let $ E $ be a simply-connected domain with as boundary a sufficiently-smooth contour $ \Gamma $ if $ y \geq 0 $ or pieces $ \Gamma _ {1} $, $ \Gamma _ {2} $, $ \Gamma _ {3} $, and $ \Gamma _ {4} $ if $ y \leq 0 $, $ \Gamma _ {1} $ and $ \Gamma _ {3} $ being the characteristics of one family, and $ \Gamma _ {2} $ and $ \Gamma _ {4} $ of the other (see Fig.). The theorem on the existence and the uniqueness of solutions of the following boundary value problems is valid in $ E $: the function $ z( x, y) $ is given on $ \Gamma + \Gamma _ {1} + \Gamma _ {4} $; the function $ z( x, y) $ is given on $ \Gamma + \Gamma _ {2} + \Gamma _ {3} $.
These problems were first studied (for $ K( y) = \mathop{\rm sgn} y \cdot | y | ^ \alpha $, $ \alpha > 0 $) by S. Gellerstedt [1] by methods developed by F. Tricomi [2] for the Tricomi problem, and represent a generalization of that problem. Gellerstedt's problem has important applications in gas dynamics with velocities around the velocity of sound. These and related problems were studied for certain multiply-connected domains and for linear equations containing lower-order terms [3].
References
[1] | S. Gellerstedt, "Quelques problèmes mixtes pour l'équation " Ark. Mat. Astr. Fysik , 26A : 3 (1937) pp. 1–32 |
[2] | F.G. Tricomi, "Integral equations" , Interscience (1957) |
[3] | M.M. Smirnov, "Equations of mixed type" , Amer. Math. Soc. (1978) (Translated from Russian) |
Comments
References
[a1] | L. Bers, "Mathematical aspects of subsonic and transonic gas dynamics" , Wiley (1958) |
Gellerstedt problem. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Gellerstedt_problem&oldid=18287