Abstract
Nonsteady aerodynamics is concerned with the time dependent fluid motion generated by (solid) bodies moving in a fluid. Normally (and as distinct from classical acoustics) the body motion is composed of a (large) steady motion plus a (small) time dependent motion. In classical acoustics no (large) steady motions are examined. On the other hand, it should be said, in most of classical aerodynamic theory small time dependent motions are ignored, i.e., only small steady perturbations from the original steady motion are usually examined. However, in a number of problems arising in aeroelasticity, such as flutter and gust analysis, and also in fluid generated noise, such as turbulent boundary layers and jet wakes, the more general problem must be attacked. It shall be our concern here.* The basic assumptions concerning the nature of fluid are that it be inviscid and its thermodynamic processes be isentropic. We shall first direct our attention to a derivation of the equations of motion, using the apparatus of vector calculus and, of course, allowing for a large mean flow velocity.
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Dowell, E.H., Curtiss, H.C., Scanlan, R.H., Sisto, F. (1989). Nonsteady aerodynamics of lifting and non-lifting surfaces. In: Dowell, E.H., Curtiss, H.C., Scanlan, R.H., Sisto, F. (eds) A modern course in aeroelasticity. Mechanics: Dynamical Systems, vol 11. Springer, Dordrecht. https://doi.org/10.1007/978-94-015-7858-5_4
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DOI: https://doi.org/10.1007/978-94-015-7858-5_4
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