Dirichlet problems for disk of the meridian plane (Q2739823)
From MaRDI portal
| This is the item page for this Wikibase entity, intended for internal use and editing purposes. Please use this page instead for the normal view: Dirichlet problems for disk of the meridian plane |
scientific article; zbMATH DE number 1646304
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Dirichlet problems for disk of the meridian plane |
scientific article; zbMATH DE number 1646304 |
Statements
16 September 2001
0 references
solenoidal potential field
0 references
axial symmetric potential function
0 references
Stokes flow function
0 references
Dirichlet problem
0 references
0 references
0.9186983
0 references
0.91797465
0 references
0.90489995
0 references
0 references
0.89738446
0 references
0.8969808
0 references
0.8886926
0 references
Dirichlet problems for disk of the meridian plane (English)
0 references
The basis characteristics of the solenoidal potential field with axial symmetry in its meridian plane are the potential \(\varphi(x,y)\) and the Stokes flow function \(\psi(x,y)\) satisfying the equations NEWLINE\[NEWLINEy\Delta\varphi (x,y)+ {{\partial\varphi}\over{\partial y}}=0,\;y\Delta \psi(x,y)-{{\partial\psi}\over {\partial y}}=0.NEWLINE\]NEWLINE The author gives effective methods for solving the Dirichlet problems for \(\varphi(x,y)\) and \(\psi(x,y)\) which are adopted for the meridian plane. New integral representations of the solutions allow to use methods of singular integral equations for the solution of the boundary value problems in the meridian plane.
0 references