Low-order parabolic theory for 2D boundary-layer stability
Author(s) -
Rama Govindarajan,
Roddam Narasimha
Publication year - 1999
Publication title -
physics of fluids
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.188
H-Index - 180
eISSN - 1089-7666
pISSN - 1070-6631
DOI - 10.1063/1.870008
Subject(s) - physics , boundary layer , ordinary differential equation , stability (learning theory) , boundary (topology) , mathematical analysis , partial differential equation , flow (mathematics) , blasius boundary layer , boundary layer thickness , boundary value problem , reynolds number , differential equation , hierarchy , order (exchange) , mechanics , mathematics , turbulence , machine learning , computer science , economics , market economy , finance , quantum mechanics
R is the local boundary-layer thickness Reynolds number, we derive a minimal composite equation that contains only those terms necessary to describe the dynamics of the disturbance velocity field in the bulk of the flow as well as in the critical and wall layers. This equation completes a hierarchy of three equations, with an ordinary differential equation correct to R~:'2 (similar to but different from the Orr-Sommerfeld) at one end, and a "full" nonparallel equation nominally correct to R~( at the other (although the latter can legitimately claim higher accuracy only when the mean flow in the boundary layer is computed using higher order theory). The LOP equation is shown to give results close to the full nonparallel theory, and is the highest-order stability theory that is justifiable with the lowest-order mean velocity profiles for the boundary layer. © 7999 American Institute of Physics. (81070-6631(99)01006-5)
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