Separated Flows and Jets 1991
DOI: 10.1007/978-3-642-84447-8_18
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Interaction Theory and Non-Uniqueness of Separated Flows Around Solid Bodies

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Cited by 11 publications
(2 citation statements)
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“…in situations where a fully attached boundary layer is forced to separate owing to the presence of a large adverse pressure gradient. Examples displaying such a branching behaviour include supersonic flows past flared cylinders (Gittler & Kluwick 1987), subsonic flows past expansion ramps and subsonic trailing edge flows (Korolev 1990). Current work indicates that this indeed leads to phenomena similar to those described here.…”
Section: Discussionsupporting
confidence: 62%
“…in situations where a fully attached boundary layer is forced to separate owing to the presence of a large adverse pressure gradient. Examples displaying such a branching behaviour include supersonic flows past flared cylinders (Gittler & Kluwick 1987), subsonic flows past expansion ramps and subsonic trailing edge flows (Korolev 1990). Current work indicates that this indeed leads to phenomena similar to those described here.…”
Section: Discussionsupporting
confidence: 62%
“…Figure 3 shows the circulation ¡ 1 as a function of c and it shows that when c exceeds c ¤ = 1:95 § 0:05, the problem has no solution. Another characteristic feature of the solution is the existence of a second lower branch, which is charac-terized by decrease in ¡ 1 and an increase in the extent of the reverse-®ow region associated with a decrease in c. It should be noted that a non-unique solution was also obtained in the theory of interaction between boundary layers and external streams in earlier studies of laminar incompressible ®ow past the leading edge of a slender airfoil in Brown & Stewartson (1983) and Ruban (1982), jet ®ows past a curved surface in Zametaev (1986) and the trailing edge of a slender airfoil in Korolev (1989), incompressible ®ow past the vertex of an obtuse angle in work of Korolev (1991), and supersonic viscous ®ow past an axially symmetric surface in Gittler & Kluwick (1987). Figures 4 and 5 compare the skin friction and the pressure distributions on the surface of the elliptic cylinder obtained for c = 1:82 and two di¬erent values of ¡ 1 and the curves 1 and 2 represent the upper and, respectively, lower branches of the solution.…”
Section: Resultsmentioning
confidence: 81%