Overview of Experiment
? Flight Conditions
– M = 0.56, 25000 feet
(Subsonic condition)
– M = 0.86, 36000 feet
(Transonic condition)
? Nose-To-Tail (N2T)
Distances
– 20, 55, 110 and 190 feet
? Nomenclature
– X-direction (longitudinal)
– Y-direction (lateral)
– Z-direction (vertical)
The subsonic flight condition (M=0.56, h=25000 feet) was selected to match pre-existing data from vortex-effect prediction codes. These codes needed to be validated to determine their utility on
future applications of AFF. Since a possible future application of AFF is for transport airplane, flight data were also acquired at M=0.86 and h =36000 feet. This transonic flight condition is
representative for that class of vehicle.
The vortex effects were also mapped at different longitudinal distances behind the leader airplane. These Nose-To-Tail (N2T) distances were monitored by the control room and maintained by the
pilots through periodic radio calls. Only the results from the subsonic condition, 55’ N2T will be presented here. 55’ is equal to the length of the F/A-18.
The reference axis system was as shown above. It should be noted that although Z is positive down, this presentation will refer to positions above the lead airplane (or high) as positive and positions
below the lead airplane (or low) as negative.
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Autonomous Formation Flight Program
NAS4-00041 TO-104
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Autonomous Formation Flight Program
NAS4-00041 TO-104
Lift and Drag Analysis
Flight Test Database
Engine Data Air Data INS Data
In-Flight Thrust Model
F
G
, F
RAM
, FE
DRAG
Wind Axis Accelerations
A
XW
, A
YW
, A
ZW
Air Data Computations
Gross Weight, V
inf
, P
o
D
est.
= T
Trail.
- J
Lead
Performance Model
D = cos( D
est
) F
G
–F
RAM
–FE
DRAG
-F
EX
C
L
, C
D
, C
Di
= C
D
–C
D0
Vortex Effect = Vortex – Baseline
% 'C
D
, % 'C
Di
, % 'WFT
Predicted Performance
(outside vortex influence)
C
L
, C
D
, C
D0
F
EX
=GW*A
XW
Performance data was determined using classical techniques. A force balance along the flight path was used to determine drag while a force balance perpendicular to that was used to determine lift:
D = cos( Dest) FG – FRAM – FEDRAG-(GW*AXW); L = sin( Dest) FG + (GW*NXW). Three primary data reduction areas feed the performance mode; 1) Air Data, 2) IFT, and 3) Accelerations.
The Air Data model computes gross weight (GW) using empty weight and the remaining total fuel accounting for crew weight. It also includes a calculation of an estimated alpha, Dest, which is based
on the trailing aircraft’s pitch angle and the lead aircraft’s flight path angle ( Dest = qtrail- Jlead). This was required because the trailing aircraft’s alpha probes are unusable during formation
flight due to localized upwash influences of the lead aircraft. Because the lead aircraft flew at steady-state conditions (constant speed and altitude), the flight path angle, Jlead, was always close
to zero.
The engine manufacturer’s IFT model was used to calculate thrust on the F404-GE-400 engines installed in the trailing F/A-18 Aircraft. The next chart describes the measurements used to run this
model. The model calculated gross thrust (FG), ram drag (FRAM) and engine throttle dependent drag, (FEDRAG). Gross thrust is the primary force the engine produces out the tail pipe, FRAM
represents the force loss due to the momentum of air, W1, entering the inlet, and FEDRAG accounts for the external drag forces associated with the engine nozzle and inlet spillage flow.
The INS was used to obtain vehicle acceleration data. This data was corrected for rotation effects due to not being mounted exactly on the center of gravity. It then was translated into the flight path
(wind axis) coordinate system. Axial acceleration was used to compute vehicle excess thrust: FEX = GW*AXW
The performance model used the information from the three paths described above to obtain lift, drag and respective coefficients. To obtain drag reduction values, data obtained during formation
flight (vortex) was compared to baseline (non-vortex) points completed in a back-to-back fashion. Some formation flight test points did not include a slide-out maneuver to obtain baseline conditions.
For these few points, baseline data were estimated based on data trends in drag related to gross weight. A simple prediction model was used to calculate baseline lift and drag values to evaluate the
reasonableness of the baseline data.
Test Point Procedure
? Pilot Procedure
– Acquire and hold position within the influence of the vortex for
30 seconds of stable data
– Engage auto-throttle velocity-hold and maintain position for
20 seconds of stable data
– Laterally slide out of position (away from lead a/c), engage
altitude-hold and stabilize outside of vortex for 20 seconds
? Technique provides direct comparison of performance data in
and out of vortex
? Use of auto-pilot and auto-throttle significantly improved
maneuver and data quality
Each test point was conducted in the same way. Once both aircraft were on condition, the trail aircraft maintained its position behind the lead aircraft for 30 sec. During this
time, the pilot of the trail aircraft was controlling every aspect of his aircraft, including throttles. Because of the transient nature of the vortex effects, especially with significant
wing overlap, the pilot’s throttle movements were, in some cases, coarse and over-corrective. This problem was exacerbated when combined with a significant longitudinal
distance like 190’ N2T, because maintaining longitudinal separation became especially difficult when the pilots did not have a good visual (close) reference.
After 30 sec of stable data, the pilot engaged the auto-throttle (ATC) velocity hold and held position for another 20 sec. More often than not, the ATC would have to be set a few
times before the N2T closure rate was small enough to call stable. After 20 sec of stable, ATC-engaged data, the control room gave the call for ‘slide out’, at which time the pilot
of the trail aircraft maneuvered laterally out of position to the right, engaged altitude-hold, and stabilized for another 20 sec outside of the vortex. The control room then gave a
‘test point complete’ call at the appropriate time.
Following a video of an example test point, an explanation as to why the test point procedure was set up in this way will be given.
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Autonomous Formation Flight Program
NAS4-00041 TO-104
Flight Test Point Matrix
4 ' 6 ' 8 ' 10 ' 12 '
-50% -25% 0% 25% 50%
(% Wingtip Separation)
Real-time feedback in cockpit using ILS needles
N2T (X) position monitored through control room calls (no
direct feedback in cockpit)
55 ft N2T
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Autonomous Formation Flight Program
NAS4-00041 TO-104
-75% -50% -25% 0% 25% 50%
Lateral Separation, Y, % wingspan
50%
25%
0%
-25%
-50%
Vertical Se
paration, Z,
%
w
i
ngspan
Condition 2
Mach 0.86
36,000 ft
Condition 1
Mach 0.56
25,000 ft
To fully map the vortex, a grid of test points, or test matrix, was created.
Several factors constrained this matrix, including:
Limited test flights available
The guidance (needle) display was limited to 60 target files.
To maximize the resolution of the vortex mapping in the most efficient manner, the matrix was based on 1/8 of an F/A-18 wingspan, or just under 5 feet.
To fully map the vortex, a grid of test points, or test matrix, was created. Because flight test time was limited, the number of matrix points had to be kept to a minimum without sacrificing the
resolution of the vortex mapping. In addition, the guidance (needle) display used by the trailing pilot to fly each test point was limited to 60 target files. Designed within these boundaries, the test
matrix was based on 1/8 of an F/A-18 wingspan (bF/A-18=37.5 ft), or about 4.7 ft. A grid of equally-spaced points in the Y- and Z- axis was then set up using this parameter. An example of such
a grid is shown above.
Autonomous Formation Flight Test Results
Summary Of Phase 0 -February 2001
Summary Of Phase 1 -August 2001
Phase 0 Control Experiment #1
Steady-State Tracking
AFF Flight 715 - February 21, 2001
2-Minute Tracking Task
High Performance Gainset
20
15
Relative Lateral Position Error (ft)
Rela
tive V
e
rtical P
o
sition
Error (f
t)
0
10
5
-20
-15
-10
-5
-20 20151050-5-10-15
Extremely Accurate Position Outside The
Vortex Demonstrated (Winter 2001).
(Experiment: Dial In –75/-75 ft Translations)
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Autonomous Formation Flight Program
NAS4-00041 TO-104
20
15
Relative Lateral Position Error (ft)
Rela
tive V
e
rtical P
o
sition
Error (f
t)
0
10
5
-20
-15
-10
-5
-20 20151050-5-10-15
AFF Flight 714 - February 21, 2001
2-Minute Tracking Task
Integral Gainset
The additional feedback of the integral of the position error in the INTEGRAL gainset was very successful at eliminating any steady-state offsets in position error. An undesired side-effect of the
integrator was larger overshoots for this gainset than for the others. However, performance and stability were still well within the acceptable region for these gains.
The HIGH PERFORMANCE gainset exhibited extremely good disturbance rejection capability. Position errors during steady-state tracking with these gains were approximately 1 foot both laterally
and vertically.
Drag Change Contour Plot
Contour plots:
? Provides a true
perspective of the vortex's
influence on vehicle
performance
Factors:
? Number of test points
? Data smoothing
– bicubic spline
? Extrapolation
– missing data points
' C
D
,
percent
M=0.56, 25,000 ft altitude, 55ft nose-to-tail
This particular contour plot (Mach 0.56, 25,000ft) contains 92 test points.
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Autonomous Formation Flight Program
NAS4-00041 TO-104
Actual Flight Test Results Validate
“Drag Bucket” Theory
Phase 1 Control
Requirement
Act
Phase 1 Control
Requirement
Phase 0 Control
Results
Drag Reduction % Drag Reduction %
Lateral Offset ( 'Y feet)
V
e
r
t
i
c
a
l
O
f
f
s
e
t
(
V
e
r
t
i
c
a
l
O
f
f
s
e
t
(
'