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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u’<br />
u<br />
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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/