Abstract
The topics of this book are the basic principles and Unit Problems of separated and vortical flow in aircraft wing aerodynamics. This chapter is devoted to short considerations of application-oriented topics. Complete literature reviews are not intended, we give compact accounts of selected topics and provide references for further reading.
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Notes
- 1.
The relation of the specific impulse \(I_{sp}\) to the specific fuel consumption b [kg/s N] of the propulsion system is \(I_{sp}\) = 1/(b g).
- 2.
The figure goes back to F. Thomas [4].
- 3.
If laminar-turbulent transition would be involved, the situation would be much more challenging.
- 4.
The shear layers leaving the trailing edges of all elements of the high-lift system are also noise sources due to the finite thickness of the edges, Sect. 6.3.
- 5.
We do not present the details of the numerical approaches. The interested reader is asked to consult the original publication [19].
- 6.
At propeller-driven subsonic aircraft with no or only small wing sweep usually no leading-edge devices are employed. Also playing a role there is the favorable interference between the propeller wake and the wing flow.
- 7.
In our discussion we assume that instead of the droop nose device (DND) inboard of the engine also a slat is present, like outboard of it.
- 8.
The higher the bypass ratio, the lower are the fuel consumption and the noise emission.
- 9.
- 10.
The classical winglet is a vertical surface at the wing tip, whereas now wing-tip extensions evolve smoothly out of the wing’s surface. Sharklet so-called are winglets solely at the aircraft of the A320 family of Airbus, see, e.g., [33].
- 11.
Airbus studies such and alternative foldable solutions.
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Hirschel, E.H., Rizzi, A., Breitsamter, C., Staudacher, W. (2021). Particular Flow Problems of Large Aspect-Ratio Wings. In: Separated and Vortical Flow in Aircraft Wing Aerodynamics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-61328-3_9
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