Abstract:
An
experimental
investigation
of the hypersonic flow
over
(i)
a wing-body
configuration,
(ii)
a
hemi-spherically blunted
cone-cylinder
body
and
(iii)
a one-half-
power-law
body has been
conducted
for M,,
=
8.2
and
Re,,
=
9.35x104
per cm.
The
tests were performed at model
incidences,
a=0,5 and
10° for flap deflection
angles,
(3
=
0,5,15,
and
25° for the wing-body.
The incidence
ranged
from
-3
to 10° for the cone-
cylinder and
-5
to 15° for the power-law
body.
(i) The
schlieren pictures showing top and side views of the model
indicate that the
body
nose shock
does
not
intersect the wing throughout the range of a under
investigation. Detailed
pressure measurements on the lower
surface of the wing and
flap
along with the liquid
crystal pictures suggest that the body
nose shock
does
not strike
the flap
surfaces either.
The
wing
leading
edge shock
is found to be
attached at a=0
and
5° but detached
at a= 10°.
The liquid
crystal pictures and surface pressure measurements
indicated
attached
flow
on the lower
surface of the wing and
flap for 13
=0 and
5°
at all values of a under
test. However
at a=
0°,
as the flap
angle
is increased to 15° the flow
separates ahead of
the hinge line. As incidence is increased the boundary layer becomes transitional giving
rise to complex separation patterns around the flap hinge line.
The
spherically
blunted body
nose causes strong entropy
layer
effects over the
wing and the trailing edge
flap. A Navier-Stokes
solution
indicated
a thick entropy
layer
of approximately constant thickness all around the cylindrical section of the body
at zero
incidence. However,
at an
incidence
of
10° the layer tapers and
becomes thinner under
the body. The
surface pressure over the wing and the plateau pressure
for
separated
flow
was
found to increase from the root to the tip. This is
partly
because
of the decrease in
local Reynolds
number across the span,
however in the present case, entropy
layer
effects also affected separation.
The
entropy
layer
effects were
found to reduce the peak
pressures obtainable on the flap. The
peak pressures, over the portion of the flap
unaffected
by
entropy
layer
effects, could
be
estimated assuming quasi two dimensional
flow.
(ii) Force
measurements were made
for the blunted
cone-cylinder alone as well as
with the delta
wing, with trailing-edge flap,
attached to it. The lift, drag,
and pitching
moment characteristics
for the cone-cylinder agree reasonably well with the modified
Newtonian theory and the N-S
results.
The
addition of a wing to the cone-cylinder
body
increases the lift
as weil as the drag
coefficient
but there is
an overall
increase in the
lift/drag
ratio.
The deflection
of a
flap from 0° to 25° increases the lift
and
drag
coefficients at all the incidences tested. However, the lift/drag
ratio
is
reduced showing
the affects of separation over the wing.
The
experimental results on the wing-body are
compared with the theoretical estimates
based
upon two-dimensional shock-expansion
theory.
(iii) The lift,
and
drag
characteristics of a one-half-power-law
body
are compared
with other existing results.
The
addition of strakes to the power-law
body
are
found to
improve its
aerodynamic efficiency without any significant change
in its
pitching
moment characteristics.