Numerical simulations are used to study laminar breakdown characteristics associated with stationary crossflow instability in the boundary-layer flow over a subsonic swept-wing configuration. Previous work involving the linear and nonlinear development of individual, fundamental modes of secondary instability waves is extended by considering the role of more complex, yet controlled, spectra of the secondary instability modes. Direct numerical simulations target a mixed mode transition scenario involving the simultaneous presence of Y and Z modes of secondary instability. For the initial amplitudes investigated in this paper, the Y modes are found to play an insignificant role during the onset of transition, in spite of achieving rather large, O(5%), amplitudes of RMS velocity fluctuation prior to transition. Analysis of the numerical simulations shows that this rather surprising finding can be attributed to the fact that the Y modes are concentrated near the top of the crossflow vortex and exert relatively small influence on the Z modes that reside closer to the surface and can lead to transition via nonlinear spreading that does not involve interactions with the Y mode. Finally, secondary instability calculations reveal that subharmonic modes of secondary instability have substantially lower growth rates than those of the fundamental modes, and hence, are less likely to play an important role during the breakdown process involving complex initial spectra.
NomenclatureA = Amplitude of crossflow instability mode or secondary instability mode, measured in terms of peak chordwise velocity perturbation and normalized with respect to freestream velocity C = Wing chord length normal to the leading edge M = Freestream Mach number m = Fourier index of frequency mode N = N factor (i.e., logarithmic amplification ratio) of linear crossflow instability or secondary instability n = Fourier index of spanwise mode U = Base flow streamwise velocity u = Perturbation streamwise velocity X = Chordwise coordinate in the direction perpendicular to the leading edge Y = Cartesian coordinate normal to the X-Z plane Z = Spanwise coordinate, i.e., the coordinate parallel to the wing leading edge DRE = Discrete Roughness Elements LSIT = Linear Secondary Instability Theory PSE = Parabolized Stability Equations Superscripts + = Wall units ∞ = Free stream init = Chordwise location where initial amplitudes of perturbations are set * Aerospace Technologist, Fei.Li@nasa.gov † Aerospace Technologist, Meelan.M.Choudhari@nasa.gov, Associated Fellow, AIAA ‡ Assistant Professor, duanl@mst.edu, Senior Member, AIAA. Downloaded by UNIVERSITY OF CAMBRIDGE on June 16, 2016 | http://arc.aiaa.org |