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A Survey of Unsteady Hypersonic Flow Problems

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u’<br />

u<br />

i;<br />

u<br />

u<br />

U<br />

li<br />

ui<br />

%<br />

v<br />

v<br />

v<br />

vf<br />

w<br />

x P<br />

x a<br />

? 8<br />

- 65 -<br />

disturbance velocity in x-direction or in &-direction<br />

transfomed quantity (equation (2.7))<br />

non-dimensional value <strong>of</strong> u (equation (2.24))<br />

horizontal component <strong>of</strong> vehicle velocity in re-entry problem<br />

ratio <strong>of</strong> u to dpR,, the circular orbital speed at radius Ri<br />

free-stream velocity or flight speed<br />

u/(gR+<br />

initial flight speed at re-entry<br />

"iA gBi+<br />

disturbance velocity cconponent in y-direction or in ~-direction<br />

non-dImensiona value <strong>of</strong> v (equation (2.24))<br />

disturbed volume <strong>of</strong> fluid in variational problem (equation (2.42))<br />

flutter speed<br />

downwash velocity at surface<br />

disturbance velocity component in z-direction or in t;-direction<br />

non-dimensional value <strong>of</strong> R (equation (2.24))<br />

weight <strong>of</strong> vehicle<br />

co-ordinate axes (Fig. 5)<br />

transformed quantity (equation (2.7))<br />

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

nonwdised co-ordinate x/C or x/X<br />

norsdised co-ordinate x/(nqse length)<br />

&l,$tance,in chord lengths, that the elastic axis <strong>of</strong> a section<br />

lies behind the leading edge<br />

value <strong>of</strong> X at centre <strong>of</strong> pressure<br />

distance, in chord lengths, that the c.g. <strong>of</strong> a section lies<br />

behind then elastic axis<br />

dimensionless amplitude <strong>of</strong> shock displacement %?h<br />

'p amplitude <strong>of</strong> displacement + curvilinear co-ordinates<br />

(Sig. 7 and equation (2.64))<br />

a/

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