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A Survey of Unsteady Hypersonic Flow Problems

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AP<br />

9<br />

P<br />

r<br />

'b<br />

F a<br />

B<br />

%<br />

R<br />

%<br />

Be<br />

Rex<br />

s<br />

9<br />

s<br />

t'<br />

t<br />

x<br />

P<br />

t<br />

T<br />

'$0<br />

Ta<br />

- 64 -<br />

P<br />

non-dimensional pressure: p = (equation (2.24))<br />

fdJ ssin'a<br />

amplitude <strong>of</strong> oscillatory non-dimensional pressure at body<br />

surface: pb (Fig. 9<br />

3PG<br />

incremental pressure<br />

and equation (2.63))<br />

fluid velocity in variational method (equation (2.42))<br />

dynamic pressure q = &p,JJ’<br />

radial cc-ordinate (Fig. 7)<br />

local radius <strong>of</strong> body (Fig. 7)<br />

-Tradius<br />

<strong>of</strong> gyration <strong>of</strong> a wing section in semi-chords: ';, = 2%<br />

d mba<br />

radius <strong>of</strong> flight path from oentre <strong>of</strong> earth<br />

initial value <strong>of</strong> radius in re-entry problem 1 Appendix III<br />

cylindrical shell radius - Appendix IV<br />

radius <strong>of</strong> spherical cap nose - Fig. 7<br />

Reynolds number based on U and 4,<br />

Reynolds number based on distance from leading edge<br />

distance along flight path in re-entry problem<br />

entropy - Appendix II<br />

representative area <strong>of</strong> vehicle - Appendices III and IV<br />

time<br />

transformed quantity (equation (2.13))<br />

non-dimensional value <strong>of</strong> t, (equation (2.23))<br />

transformed quantity (equation (2.36))<br />

thickness <strong>of</strong> panel or shell - Appendix IV<br />

local temperature (OR)<br />

free-stream temperature<br />

stream temperature immediately behind shook wave<br />

Appendix II

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