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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

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