INTRODUCTION
|
The AeroRocket wind tunnel has been used
to determine center of pressure location (XCp) and zero-degree
drag coefficient (Cd) of spool rocket models having various plate-separation
to plate-diameter ratios (L/D). Five spool rocket wind tunnel
models were tested having L/D ratios of 1, 1.33, 1.67, 2 and
3. The ratio of the separation distance (L) to plate diameter
(D) is the value of L/D used to correlate Cd and XCp for data
presentation. To avoid wind tunnel wall interference effects
the diameter (D) of the spool rocket end-plates are 1.5 inches
and fabricated using 1/32" thick aircraft plywood to more
accurately simulate the plate-diameter to plate-thickness ratio
used to fabricate most practical spool rockets. The end-plates
are supported by a single 3/8" diameter (d) wooden dowel
or cylindrical body having lengths of 1.5", 2", 2.5",
3" and 4.5" for each of the five models tested in the
AeroRocket wind tunnel. Figure-1 schematically displays the force
balance system used to determine Cd of the spool rocket models
in the AeroRocket wind tunnel. Figure-5 displays the various
spool rocket models tested to determine drag and center of pressure
location. |

Figure 1. General schematic
of the Force Balance System
DRAG COEFFICIENT (Cd)
|
Displacement in the axial (drag) and vertical
(lift) directions are measured using the two load cells labeled
DRAG and LIFT respectively in Figure-1 and then
converted to drag and lift forces in Newtons using the Vernier
CBL-2 computerized data acquisition system. The force balance
system pictured above is designed to separate the aerodynamic
forces and the associated displacements in the axial and vertical
directions when the weight on the force-balance plate causes
the model to be freely suspended. Spool rocket drag coefficient
(Cd) has been plotted in the form presented in Figure-2a and
Figure-2b as a function of L/D. The AeroRocket wind tunnel Cd
data (red dots) in Figure-2a are plotted with Cd data (blue line)
from an independant source referenced in the report dealing with
drag of circular plates. The report also introduces a curve-fit
approximation of spool rocket Cd verses L/D over the range of
L/D=0.5 to L/D =3.5. Figure-2b presents a representation of the
curve-fit data for spool rocket Cd verses L/D. The actual report
labels all axes. |

Figure-2a, Spool rocket Cd verses L/D (red dots) and independant
data

Figure-2b, Spool rocket Cd verses L/D (red dots) and curve-fit
approximation

Figure 3, Typical drag
coefficient (Cd) measurement, L/D = 2 shown

Figure 4, Typical drag
coefficient (Cd) measurement, L/D = 2 shown
CENTER OF PRESSURE (XCp)
|
Center of pressure measurements are performed
using a special XCp-Caliper that secures the model in the wind
tunnel test section using two opposing low friction points. Figure-5
displays the spool rocket models tested (L/D = 3 not pictured)
and the XCp-Caliper used to secure the spool models during center
of pressure measurement. The models are secured by the cylindrical
sting placed behind the rear plate. Figure-6 illustrates the
L/D = 2 spool rocket model being tested in the AeroRocket wind
tunnel. The model in this configuration is stable because the
support point is ahead of the actual center of pressure. The
actual center of pressure location (XCp) is determined by moving
the sting support location rearward until the model becomes unstable
and "noses over" to one side or the other when the
wind tunnel is operating. Figure-6 further illustrates how the
spool rocket model is secured in place during center of pressure
location testing. Please notice the pitot tube used to measure
the difference between static pressure and dynamic pressure for
determining flow velocity in the wind tunnel. An analog velocity
meter is used to convert the resulting pressure differential
to test section flow velocity in feet per minute. |

Figure-5, L/D = 2 Model
On XCp-Caliper and spool models (L/D=3 not pictured)

Figure 6. Center of pressure
measurement using XCp-Caliper (L/D = 2)
|
Figure-7 displays the AeroRocket wind tunnel
results for center of pressure (XCp/D) location verses L/D for
the five spool rocket models tested. The center of pressure (XCp)
is normalized by the plate diameter, (D). Normalization is performed
to generalize the results to any size spool rocket design. The
AeroRocket wind tunnel XCp/D data (red dots) in Figure-7 are
plotted along with a logarithmic curve-fit approximation of spool
rocket XCp/D verses L/D over the range of L/D = 0.5 to L/D =
3.5. |

Figure-7, Spool rocket XCp verses L/D (red dots) and curve-fit
approximation
WHY IS A STING REQUIRED FOR CENTER OF PRESSURE MEASUREMENT
|
For a spool rocket the center of pressure (XCp)
is located behind the rear plate of the model. Therefore, it
is necessary to support the spool rocket behind the back plate
when attempting to determine center of pressure location. To
support the model for center of pressure measurement a support
sting was added to the rear of each spool rocket model. The following
discussion describes why the presence of the cylindrical support
sting does not affect the center of pressure location of the
model being tested.
For angles of attack less than 10 degrees the normal forces acting
on any cylindrical body are small and the effect of a support
sting on center of pressure location can be neglected as stated
in TIR-33. In other words, the normal forces acting on a cylindrical
body, that could contribute to center of pressure movement, are
seen to disappear for angles of attack less than 10 degrees.
Therefore, the presence of a cylindrical support sting inserted
behind the model does not alter the center of pressure location
of a model being tested in the wind tunnel. Therefore, the effect
of a cylindrical support sting attached to the rear of any wind
tunnel model on center of pressure location is very small because
the normal forces acting on a cylindrical body are small for
angles of attack less than 10 degrees. This discussion is important
because the measurement of center of pressure location (XCp)
relies on the placement of a cylindrical support sting behind
the rear plate of the spool rocket model. The support sting and
spool rocket model combination are held securely in place during
center of pressure measurement by the two opposing points of
the XCP-Caliper illustrated in Figure-5 and Figure-6. Figure-6
illustrates the L/D = 2 spool rocket model being tested in the
AeroRocket wind tunnel. The model in this configuration is stable
because the support point is ahead of the actual center of pressure.
The actual center of pressure location (XCp) is determined by
moving the sting support location rearward until the model becomes
unstable and "noses over" to one side or the other
when the wind tunnel is operating. Figure-5 and Figure-6 further
illustrate how the spool rocket model is secured in place during
center of pressure location testing. Please notice the pitot
tube used to measure the difference between static pressure and
dynamic pressure for determining flow velocity in the wind tunnel.
An analog velocity meter is used to convert the resulting pressure
differential to test section flow velocity in feet per minute. |
APPLICATION TO FULL SIZE SPOOL ROCKETS
|
By the principal of similitude a wind tunnel
model needs to be similar in shape and have the same Reynolds
number (U*D/v) to accurately model the flight characteristics
of any "similar" full size rocket. In addition, the
correlation of circular plate wind tunnel measurements to other
full size spool rocket configurations using circular plates is
enhanced by the fact that above Reynolds number 1,000 and up
to Reynolds number 1.0E7 the drag coefficient of disks and plates
is practically constant and approximately equal to 1.17 for a
single circular plate in normal flow. In other words for a circular
plate the transition from laminar flow to turbulent flow occurs
above Reynolds number 1,000 and the associated drag coefficient
(Cd) for a flat circular plate in turbulent flow remains constant
up to the highest Reynolds number ever tested, approximately
1.0E7. The spool rocket wind tunnel models tested in the AeroRocket
wind tunnel had an average Reynolds number of 50,550. Because
Reynolds numbers are well above 1,000 and below 1.0E7 the results
are representative of the region of spool rocket air flow where
Cd is constant and predictable over a wide range of velocity.
This relationship between Cd and Reynolds number makes possible
the extension of these wind tunnel test results to any spool
rocket that has Reynolds number and shape similar to the spool
rocket models tested. |

Figure 8, AeroRocket Wind
Tunnel and various models from past work
|
SPECIAL NOTICE
NO PART OF THIS REPORT MAY BE COPIED OR TRANSFERRED TO ANOTHER
USER WITHOUT THE WRITTEN CONSENT OF JOHN CIPOLLA/AEROROCKET.
ALSO, WHEN PURCHASING AEROROCKET SOFTWARE AND REPORTS THE USER
IS AGREEING THE SOFTWARE/REPORT IS SOLD AS IS AND NO WARRANTY
IS EXPRESSED OR IMPLIED. THE USER TAKES COMPLETE RESPONSIBILITY
FOR USING THE SOFTWARE/REPORT AND PROPERLY INTERPRETING THE RESULTS. |
For more information concerning the
Spool Rocket Wind Tunnel Report please contact AeroRocket at
aerocfd@aerorocket.com.
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