Abstract
This chapter is devoted to an introduction to some of the concepts used when dealing with separated and vortical flow.
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Notes
- 1.
Regarding the geometry of actual trailing and leading edges see Chap. 6.
- 2.
This momentum thickness concept does not hold for three-dimensional boundary layers. There the momentum-flow displacement thickness is the physically meaningful concept [5]. Nevertheless, the two-dimensional momentum thickness concept suffices for our considerations, as long as the treated flow is not too strongly three-dimensional.
- 3.
If locally the inverse of the boundary-layer thickness \(\delta \) is of the order of magnitude of the largest of the principal surface curvatures radii \(R_{i}\), the pressure gradient is no more small due to the centrifugal forces induced by the surface curvature [5]. This is the best known boundary-layer higher-order effect. It can be treated with second-order boundary-layer theory.
- 4.
External means at the outer edge of the boundary layer.
- 5.
This contradicts van Dykes statement that a wake exerts a first-order influence even in the flow upstream [16]. Of course, the integral forces and moments, which the flow exerts on the body, are affected by separation.
- 6.
When in the late 1930s the potential of airbreathing jet propulsion emerged—recognized at that time predominantly in Germany [17]—the drag divergence was a matter of very high concern.
In Germany up to 1945 frantic work at research organizations and in aircraft industry was conducted in order to shift in particular the drag divergence to as high as possible (sub-sonic) flight Mach numbers. Connected to the supercritical airfoil are the names K.H. Kawalki and B. Göthert, to the swept wing the names A. Busemann, H. Ludwieg, A. Betz, to the delta wing A. Lippisch, and to the area rule O. Frenzl. The area rule later was confirmed with the equivalence theorem by F. Keune and K. Oswatitsch (1953). An overview of the work is given in [17] and a very detailed account in [18].
When the war ended, the outcome of this work, which in Germany barely came to an application, found its way to the Allies. In [17] a short section “Transfer of the German Aeronautical Knowledge After 1945” is included, details regarding the American acquisition of data are given in [19]. Large research and development efforts in a short time then changed the geometrical appearance of all kind of aircraft. For the USA see in this respect the publication of J.D. Anderson, Jr., “The Airplane: A History of Its Technology” [20].
- 7.
The zero-lift drag is the drag of the aircraft without the induced drag.
- 8.
The shock wave terminates orthogonally to the airfoil’s surface, although at the boundary-layer edge particular phenomena can be present. For all pre-shock Mach numbers this leads to a reduction of the unit Reynolds number and hence to a thickening of the boundary layer.
- 9.
In the literature often the lower critical Mach number \(M^{*}_{\infty ,l}\) is distinguished from the upper critical Mach number \(M^{*}_{\infty ,u}\). At \(M^{*}_{\infty ,l}\) supersonic flow begins to appear at the body, at \(M^{*}_{\infty ,u}\) the flow past the body is fully supersonic, at a blunt-nosed body except for the subsonic region at the nose.
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Hirschel, E.H., Rizzi, A., Breitsamter, C., Staudacher, W. (2021). Separation: Some Relevant Boundary-Layer Properties, Interaction Issues, and Drag. In: Separated and Vortical Flow in Aircraft Wing Aerodynamics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-61328-3_2
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