2001
DOI: 10.1016/s0169-5983(00)00019-8
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Three-dimensional inviscid waves in buoyant boundary layer flows

Abstract: The stability of weakly three-dimensional buoyancy-driven boundary layers to travelling waves is considered. It is shown that in the absence of cross ow inviscid modes are unstable and, as the degree of cross ow is increased, the short waves are the ÿrst to be stabilised -longer waves require an enhanced level of three-dimensionality of the basic ow for stabilisation. A combination of asymptotic and numerical techniques are used to provide a complete description of the inviscid modes over the whole wavenumber … Show more

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Cited by 2 publications
(2 citation statements)
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“…where the similarity variable η =Ỹ x (m−1)/2 , provided the far-field flow is u e (x) = x m and the wall temperature T w (x) = x (5m−1)/2 . The functions f, g, and q are given by the solution of a sixth-order system of differential equations (see [22] for details). A typical form of the streamwise flow is illustrated in Figure 1; here m = 1/3 and corresponds to the flow past a swept right-angled wedge.…”
Section: The Basic Flowmentioning
confidence: 99%
“…where the similarity variable η =Ỹ x (m−1)/2 , provided the far-field flow is u e (x) = x m and the wall temperature T w (x) = x (5m−1)/2 . The functions f, g, and q are given by the solution of a sixth-order system of differential equations (see [22] for details). A typical form of the streamwise flow is illustrated in Figure 1; here m = 1/3 and corresponds to the flow past a swept right-angled wedge.…”
Section: The Basic Flowmentioning
confidence: 99%
“…A forward integration has been done by Steinrück (2001) and Lagree (2001). However, regarding stability, interesting phenomena occur which have been investigated by Denier, Stott & Bassom (2001).…”
Section: Introductionmentioning
confidence: 99%