Spatial direct numerical simulation of boundary-layer transition mechanisms: Validation of PSE theory
Author(s) -
R. D. Joslin,
Craig L. Streett,
ChauLyan Chang
Publication year - 1993
Publication title -
theoretical and computational fluid dynamics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.817
H-Index - 59
eISSN - 1432-2250
pISSN - 0935-4964
DOI - 10.1007/bf00418777
Subject(s) - direct numerical simulation , mechanics , adverse pressure gradient , instability , boundary layer , laminar flow , turbulence , physics , flow (mathematics) , wavenumber , mathematics , flow separation , classical mechanics , reynolds number , optics
A study of instabilities in incompressible boundary-layer flow on a flat plate is conducted by spatial direct numerical simulation (DNS) of the Navier-Stokes equations. Here, the DNS results are used to evaluate critically the results obtained using parabolized stability equations (PSE) theory and to study mechanisms associated with breakdown from laminar to turbulent flow. Three test cases are considered: two-dimensional Tollmien-Schlichting wave propagation, subharmonic instability breakdown, and oblique-wave breakdown. The instability modes predicted by PSE theory are in good quantitative agreement with the DNS results, except a small discrepancy is evident in the mean-flow distortion component of the two-dimensional test problem. This discrepancy is attributed to far-field boundary-condition differences. Both DNS and PSE theory results show several modal discrepancies when compared with the experiments of subharmonic breakdown. Computations that allow for a small adverse pressure gradient in the basic flow and a variation of the disturbance frequency result in better agreement with the experiments.
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