A Survey of Unsteady Hypersonic Flow Problems
A Survey of Unsteady Hypersonic Flow Problems
A Survey of Unsteady Hypersonic Flow Problems
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- 66 -<br />
instantaneous angle <strong>of</strong> attack<br />
amplitude <strong>of</strong> oscillatory angle <strong>of</strong> attack<br />
mean angle <strong>of</strong> attack<br />
4iFT<br />
ratio <strong>of</strong> specific heats<br />
flight path angle to local horizontal<br />
Appendix III<br />
flight path angle at start <strong>of</strong> re-entry<br />
1<br />
quantity specified by the largest <strong>of</strong> the thickness ratio, mean<br />
incidence <strong>of</strong> body or surface, and the dimensionless amplitude<br />
<strong>of</strong> the time-dependent motion - Appendix II<br />
the thickness ratio <strong>of</strong> aer<strong>of</strong>oil section - Appendix IV<br />
apparent boundary layer thickness - wall to 9% free-stream<br />
velocity point (Figs. 64 and 65)<br />
prefix denoting a small variation <strong>of</strong> a quantity in the variational<br />
problem (Appendix IV)<br />
semi-apex angle <strong>of</strong> delta wing<br />
density ratio across shock wave<br />
cc-ordinate axis (Fig. 6)<br />
non-dimensional value <strong>of</strong> c (equation (2.23)) 3<br />
= oh/wf (AppendFx IV)<br />
co-ordinate axis (Fig. 6)<br />
non-dimensional value <strong>of</strong> q (equation (2.23))<br />
Appendix II<br />
steady surface slope measured fran chordline or body axis<br />
value <strong>of</strong> 8 at the nose<br />
order <strong>of</strong> magnitude <strong>of</strong> perturbations<br />
relative density <strong>of</strong> vehicle (equation (3.1))<br />
mass ratio <strong>of</strong> wing<br />
= m/4bap for tnc-dimensional sectionj m is mass per<br />
unit span b = g/2<br />
= &basp for a wingi m is mass <strong>of</strong> wing b = z/2<br />
s = span <strong>of</strong> wing<br />
local viscosity<br />
viscosity <strong>of</strong> free stream