By Th. Von Kármán
Read or Download Advances in Aeronautical Sciences. Proceedings of the Second International Congress in the Aeronautical Sciences, Zürich, 12–16 September 1960 PDF
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Additional info for Advances in Aeronautical Sciences. Proceedings of the Second International Congress in the Aeronautical Sciences, Zürich, 12–16 September 1960
For its calculation in the classical way we have to perform the mixing in a reversible way which can be done, at least on principle, by the application of semi-permeable pistons. Heat has to be added and work is done. If we use one mole of each gas for example, entropy is increased by As = R - 2 · In 2 as a simple calculation shows. j Ί. Wire mesh screen Gae supply L k Icorni igno- rieren ry w modeler FIG. 20. Experiment of Kantrowitz, showing loss of stagnation pressure in consequence of an entropy increase by relaxation.
S Madrid 1958), de J . - P . GUIRAUD 46 sorte que la formule précédente devrait être appelée formule de NewtonBusemann-Hayes. Cette formule est suffisamment simple pour se laisser mener jusqu'aux applications numériques dans quelques cas. Nous citerons trois exemples typiques: force globale à l'intrados d'une aile mince(28), efforts globaux agissant sur des obstacles de révolution sous faible incidence*28,29), cônes circulaires sous incidence(43). Ce dernier cas est particulièrement simple et Laval(43) a pu exprimer la finesse d'un cône d'ouverture 20 par la formule: f = 1£λ \ *lmaX cos (20) = j^sinfl 3cos(20)—i Après avoir mentionné quelques applications de la théorie, il est instructif d'en discuter les limitations.
Values of the state variables inside a normal shock after R. Becker. L is free path length. The different terms of the energy-equation are drawn separately in the last diagram. 85 · 10~4 — - — . cm2 cm sec άΤ j 4 aw\ aw , , d 2 T equation: c y . ^ . _ = - ( p - y ^ - ) . _ + Energy A . — Thomas has included the variability of the coefficients of heat conduction and viscosity (μ ~ \/Τ) and he found values for the thickness little differing from Becker's(17). 8 The finite limit comes from the indefinite growing of viscosity and heat conductivity with shock strength.