Degeneracy in the Blasius problem
The Navier-Stokes equations for the boundary layer are transformed, by a similarity transformation, into the ordinary Blasius differential equation which, together with appropriate boundary conditions constitutes the Blasius problem, $$ f'''(eta )+frac{1}{2}f(eta )f'...
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Texas State University
2007-05-01
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Online Access: | http://ejde.math.txstate.edu/Volumes/2007/79/abstr.html |
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doaj-d6f3877da4fd4b2080d25abcdff623932020-11-24T23:32:59ZengTexas State UniversityElectronic Journal of Differential Equations1072-66912007-05-0120077918Degeneracy in the Blasius problemFaiz AhmadThe Navier-Stokes equations for the boundary layer are transformed, by a similarity transformation, into the ordinary Blasius differential equation which, together with appropriate boundary conditions constitutes the Blasius problem, $$ f'''(eta )+frac{1}{2}f(eta )f''(eta)=0,quad f(0)=0,; f'(0)=0,; f'(infty )=1. $$ The well-posedness of the Navier-Stokes equations is an open problem. We solve this problem, in the case of constant flow in a boundary layer, by showing that the Blasius problem is ill-posed. If the second condition is replaced by $f'(0)=-lambda $, then degeneracy occurs for $0<lambda <lambda _{c}simeq 0.354$. We investigate the problem analytically to explain this phenomenon. We derive a simple equation $g(alpha ,lambda )=0$, whose roots, for a fixed $lambda $, determine the solutions of the problem. It is found that the equation has exactly two roots for $0<lambda <lambda _{c}$ and no root beyond this point. Since an arbitrarily small perturbation of the boundary condition gives rise to an additional solution, which can be markedly different from the unperturbed solution, the Blasius problem is ill-posed.http://ejde.math.txstate.edu/Volumes/2007/79/abstr.htmlNavier-Stokes equationsBlasius problemdegeneracyWang equationwell-posed problemill-posed problem |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Faiz Ahmad |
spellingShingle |
Faiz Ahmad Degeneracy in the Blasius problem Electronic Journal of Differential Equations Navier-Stokes equations Blasius problem degeneracy Wang equation well-posed problem ill-posed problem |
author_facet |
Faiz Ahmad |
author_sort |
Faiz Ahmad |
title |
Degeneracy in the Blasius problem |
title_short |
Degeneracy in the Blasius problem |
title_full |
Degeneracy in the Blasius problem |
title_fullStr |
Degeneracy in the Blasius problem |
title_full_unstemmed |
Degeneracy in the Blasius problem |
title_sort |
degeneracy in the blasius problem |
publisher |
Texas State University |
series |
Electronic Journal of Differential Equations |
issn |
1072-6691 |
publishDate |
2007-05-01 |
description |
The Navier-Stokes equations for the boundary layer are transformed, by a similarity transformation, into the ordinary Blasius differential equation which, together with appropriate boundary conditions constitutes the Blasius problem, $$ f'''(eta )+frac{1}{2}f(eta )f''(eta)=0,quad f(0)=0,; f'(0)=0,; f'(infty )=1. $$ The well-posedness of the Navier-Stokes equations is an open problem. We solve this problem, in the case of constant flow in a boundary layer, by showing that the Blasius problem is ill-posed. If the second condition is replaced by $f'(0)=-lambda $, then degeneracy occurs for $0<lambda <lambda _{c}simeq 0.354$. We investigate the problem analytically to explain this phenomenon. We derive a simple equation $g(alpha ,lambda )=0$, whose roots, for a fixed $lambda $, determine the solutions of the problem. It is found that the equation has exactly two roots for $0<lambda <lambda _{c}$ and no root beyond this point. Since an arbitrarily small perturbation of the boundary condition gives rise to an additional solution, which can be markedly different from the unperturbed solution, the Blasius problem is ill-posed. |
topic |
Navier-Stokes equations Blasius problem degeneracy Wang equation well-posed problem ill-posed problem |
url |
http://ejde.math.txstate.edu/Volumes/2007/79/abstr.html |
work_keys_str_mv |
AT faizahmad degeneracyintheblasiusproblem |
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1725532389984174080 |