Development of the HFV-3X
Hypersonic Flight
Vehicle

HFV-3X Hypersonic
Aircraft Wind Tunnel Model

HFV-3X Hypersonic
Aircraft
AeroWindTunnel
Wire Frame Design
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Introducing
the HFV-3X, AeroRocket's version of the DARPA HTV-3X known as
the Blackswift represents AeroRocket's proposal for a
new hypersonic spacecraft capable of flight to 300,000
feet and top speed from Mach 5 to Mach 10. A
miniature subsonic wind tunnel model of the
new HFV-3X has been
fabricated for experimental determination of CD,
CL, CLa, CMa
and L/D for use with
AeroWindTunnel
a subsonic and supersonic aircraft design program. Supersonic drag and lift properties of the
HFV-3X design will be investigated using AeroRocket's new supersonic
blow-down
wind tunnel. Please see the
Wikipedia article about the HTV-3X that contains DARPA video
and other interesting information about this proposed space plane.
HFV-3X Design
(348 KB
Download - Password provided after purchase):
WinZip file containing techniques used to fabricate the 9 inch long HFV-3X
subsonic wind
tunnel model, HFV-3X wind tunnel model templates, full size
orthographic image of the HFV-3X and an
AeroWindTunnel
screen shot showing CD verses Mach number for the HFV-3X. More information
will be included in the download as development of the HFV-3X continues... |
RESOURCES AVAILABLE FOR THE DEVELOPMENT OF
THE HFV-3X
SUPERSONIC/HYPERSONIC FLIGHT VEHICLE CONCEPT |
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SUBSONIC WIND TUNNEL
The
AeroRocket subsonic wind tunnel
is a suction system powered by a two speed 1/3 horsepower fan.
The test section is 7 inches wide x 10 inches high x 16 inches long. A research quality pitot
tube measures the difference between static and dynamic
pressure in the test section. The
resulting differential determines flow velocity using an analog velocity
meter. Small models that represent large designs are
routinely tested in the AeroRocket wind tunnel. |
SUPERSONIC BLOW-DOWN WIND TUNNEL (1" DIAMETER)
The new AeroRocket 1" diameter supersonic blow-down wind tunnel performs
drag measurements up to Mach 3.
AeroRocket's expertise in the fabrication
of miniature wind tunnel models makes possible the measurement
of supersonic Cd for designs ranging from
simple high power rockets to the complex HTV-3X. This
new supersonic wind tunnel has already been used to determine drag
coefficient of the HTV-3X. These measurements determined drag coefficient for the HTV-3X to
be: Cd
= 0.1016 at M = 2.64. |
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Miniature HTV-3X Supersonic Blow-Down Wind Tunnel Model |

Close-up view of the new 1"
diameter Supersonic Blow-Down Wind Tunnel |
|
HTV-3X BLOW-DOWN
WIND TUNNEL RESULTS |
Cd, Blow-Down Wind
Tunnel
Max. Frontal Reference Area |
Cd, Ideal
Wave Drag
Equation
Max. Frontal Reference Area |
|
Cd = 0.1016 @ M = 2.64 |
Cd = 0.0906 @ M =
2.64 |
HTV-3X MODEL
Length = 12.7 mm
Width = 6.35 mm
Thickness = 2.388 mm
Smax = 15.161 mm2
Pstatic = 0.106 atm
P0 = 2.241 atm
Blockage Factor = 2.992%
q = 1/2
g
Pstatic Mn2 = 0.518 atm |
FULL SIZE HTV-3X
Lb = 15.62 m
Smax = 8.128 m2
Swing = 52.628 m2
Savg = 5.159 m2
Ewd = 1.5
LLE = 54.44 deg
Ainlet = 2.0 m2 |
Table
requires browser to display Greek letters (L
and
g
) |

Testing The miniature HTV-3X in the new 1" Blow-Down Wind
Tunnel at M = 2.64.
NOTE: Cd measurements using the new supersonic wind
tunnel have been refined because in previous tests the model
was not securely positioned on the sting causing unwanted
AOA. |
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AeroWindTunnel Cd vs. Mn
(blue line) and Cd
at Mn = 2.64
(red dot)
using
the new 1" inside-diameter Supersonic
Blow-Down Wind Tunnel |
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For the plot
illustrated on the left, data was generated using
AeroWindTunnel
with Surface-Roughness-None to plot Cd vs. Mn
(blue line).
Cd vs. Mn
(red dots) for the plot
illustrated on the left was generated
using the supersonic/hypersonic wave drag equation (CDwave)
added to base drag (Cdbase) then
plotted verses
AeroWindTunnel
results
(blue line). |
|
The
Computational Fluid Dynamics (CFD) pressure-contour plot
displayed to the right is the result of two separate
VisualCFD analyses. One two-dimensional analysis in the
plot represents the upper-half of the HTV-3X airframe
and the other two-dimensional analysis in the plot
represents the lower-half of the airframe to form the entire
Mach 2.64 supersonic flow pattern. The drag coefficient, Cd
for two-dimensional flow was converted to three-dimensional
Cd using a proprietary approach attained by over 20
years of aerospace engineering experience. Using this
proprietary approach the following Cd results were obtained
for the HTV-3X using VisualCFD.
|
Cd_0 |
2-D VisualCFD RESULTS |
|
0.418 |
Without
Ainlet. Cdbase
and Cdfriction included. |
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0.301 |
With
Ainlet. Cdbase
and Cdfriction included. |
|
0.394 |
Without
Ainlet. Cdbase
and Cdfriction removed. Cdwave |
|
0.283 |
With
Ainlet. Cdbase
and Cdfriction removed. Cdwave |
|
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Cd_0 |
2-D TO
3-D CONVERSION RESULTS |
|
0.197 |
Without
Ainlet. Cdbase
and Cdfriction included. |
|
0.141 |
With
Ainlet. Cdbase
and Cdfriction included. |
|
0.185 |
Without
Ainlet. Cdbase
and Cdfriction removed. Cdwave |
|
0.133 |
With
Ainlet. Cdbase
and Cdfriction removed. Cdwave |
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PRODUCTS |
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MISSION
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Copyright © 1999-2010 John Cipolla/AeroRocket |