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2003
DOI: 10.1017/s0022112003004786
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Receptivity of a supersonic boundary layer over a flat plate. Part 1. Wave structures and interactions

Abstract: This paper is the first part of a two-part study on the mechanisms of the receptivity to disturbances of a Mach 4.5 flow over a flat plate by using both direct numerical simulations (DNS) and linear stability theory (LST). The main objective of the current paper is to study the linear stability characteristics of the boundary-layer wave modes and their mutual resonant interactions. The numerical solutions of both steady base flow and unsteady flow induced by forcing disturbances are obtained by using a fifth-o… Show more

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Cited by 232 publications
(227 citation statements)
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References 34 publications
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“…For the Reynolds number of his example, this additional viscous solution is damped, and it is analogous to the Mode F mentioned in prior sections. We would like to point out that [MZ03a,MZ03b] and [ZM02] refer to Mode F as Mode I and refer to Mode S, not as a single family, but rather to the parts that comprise the family (Mack's first mode, second mode, etc. ).…”
Section: Discussionmentioning
confidence: 99%
“…For the Reynolds number of his example, this additional viscous solution is damped, and it is analogous to the Mode F mentioned in prior sections. We would like to point out that [MZ03a,MZ03b] and [ZM02] refer to Mode F as Mode I and refer to Mode S, not as a single family, but rather to the parts that comprise the family (Mack's first mode, second mode, etc. ).…”
Section: Discussionmentioning
confidence: 99%
“…Direct numerical simulations (DNS) of receptivity of a flat-plat boundary layer were conducted by Ma & Zhong (2003a,b, 2005 and Balakumar (2003Balakumar ( , 2005. These simulations, in which shocks are present and accounted for, show that in the presence of free-stream acoustic, vortical and entropy disturbances, first and second modes are excited.…”
Section: Introductionmentioning
confidence: 99%
“…Our understanding of different instability mechanisms, and of different transition processes in shear layers, have greatly improved in the last several decades. [1][2][3][4][5][6][7][8] Transition-prediction methods, however, have not made much progress 9 . The main difficulty is due to the nature of the transition process itself, which depends on the boundary layer characteristics and on the frequency and wave number distributions of the disturbances that enter the boundary layer.…”
Section: Introductionmentioning
confidence: 99%