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NASA-TM-88442
Iq~(p D{J (q19:l
https://ntrs.nasa.gov/search.jsp?R=19860019492 2020-05-26T12:34:45+00:00Z
NASA TECHNICAL MEMORANDUM NASA TM-88442
TESTS WITH THREE-DIMENSIONAL ADJUSTMENTS IN THE RECTANGULAR WORKING SECTION OF THE FRENCH T2 WIND TUNNEL, WITH AN
AS 07-TYPE SWEPT-BACK WING MODEL
A. Blanchard, M. J. Payry, J. F. Breil
Translation of "Essais 'd'adaptation tridirnensionnelle' de la veine rectangulaire de la soufflerie T2, en presence d'une rnaquette d'aile en fleche du type AS 07," Rapport Technique OA 34/3075 (DERAT 12/5015 ON), O.N.E.R.A., Centre d'Etudes et de Recherches de Toulouse, November 1985, pp. 1-24 (plus figures).
,LANGLE.Y RESEARCH CENTER LIBRARY, NASA
HAMPTON, VIRGINIA
NATIONAL AERONAUTICS AND SPACE ADMINISTRATION WASHINGTON, DC 20!546 JULY 1986
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I :1. Go,"c,nnu,,' ,",CCe. ,ion No'. 3. ~·.c;,..,.n'. C01cdop t,,,,, I 442 1. Rc:po., NC'..
NASA TM-88
I.. T ;tl. one! :)u h.;.,. ADJUSTMENT THE FRENCH
CK WING.,_
S IN T2
TESTS WITH THREE-DIMENSIONAL . 5. R., ... D... ~ THE RECTANGULAR WORKING SECTION OF P."o.~~pl ~'P~:~~;on Cod. WIND TUNNEL WITH·AN AS 07-TYPE SWEPT- 6.
I:::JQDEI, E. p •• r.,,,ninp Q'90ni2ct.on R.port No
A. Blanchard, J. Payry, Breil 7. ,l..u.ho'(.)
M. J. F.
10. Wo.~ Un;' No.
ll. Con"Clc~ o. C,ont No.
9. Pc.ro'min~ O.,O"'\I&Ol;on Nom. one! J...Je •••• NASW-4006 The Corpor 1102 Arrot Pittsburgh
ate ~ortl, inc. 13. Type 01 F\.pO,1 on.! P.,io~ co .... ,.c
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National A Washington
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'«",cncy Nom. Or'll! Acc, ••• eronautics and Space , DC 20546
Translation
Administration 1,(. 5pon,o"n, Apency Co~.
cry NOlet Translation of "Essais 'd'adaptation tridimensionnelle' de la veine rec1: fleche du O.N.E.R.A. 1-24 (plus
angulaire de la soufflerie T2, en presence d'une maquette type AS 07, " Rapport Technique OA 34/3075 (D~HAT 12/5015 , Centre d'Etudes et de Recherches de Toulouse, November figures).
d'aile en DN) , 1985, pp.
1~. Ab.troc' This report presents the results obtained on 'the AS 07 wing and the working se "non-adapt which comp
ction walls for three types of configurations .. The first, called ed, .. corresponds to the divergent upper and lower rectilinear walls ensate for limit layer thickening. It can serve as a basis for com·· calculations. The second configuration corresponds to wall shapes from calculation's which tend to minimize interference at the level of
ge'.
. plete flow determined the fuse;I.-a tion," use determine not suffie dinated :wi
Finally., the third configuratiotl, called "two-dimensional: adap.ta-s the st~ndard method, for T2 profile tests. This case was tested to the influence of wall shape and error magnitude. These results are ient to validate' the three-dimensional adaptation; they must be coo;r-th caiculations or wi,th ' un 1 imi ted atmosphere tests.
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TABLE OF CONTENTS
NOTATION
1 - INTRODUCTION
2 - ADAPTATION PRINCIPLE
2.1 Two-dimensional adaptation
2.2 Three-dimensional adaptation
3 - EXPERIMENT EQUIPMENT
3.1 Working section equipment
3.2 Mounting the wing
3.3 Acquisition and examination program
4 .- SUMMARY OF TESTS MADE
5 - CON'I'ROL TESTS
5.1 Angling by wall rotation
5.2 Iteration convergences
5.2.1 Three-dimensional adaptation
5.2.2 Two-dimensional adaptation
5.3 Non /2.0/3.0 comparison
5.4 Visualizations
6 - SYSTEMATIC TESTS
7 - CONCLUSION
REFERENCES
LIST OF FIGURES
ANNEX 1 - Cz
2 - Kp
3 - File listing
4
5
7
8
8
9
9
10
11
13
17
17
17
17
18
18
20
21
22
24
25
3
NOTATION
::] Cartesian coordinates in the reference working section
Zp (porthole axis)
Y
X
Z
)
Cartesian coordinates in the wing reference (leading
edge to socket)
C Profile chord of the wing section considered
Angle of the model (fuselage axis)
Mo Infinite Mach upstream of the flow
M Local Mach (wing or wall)
Pressure coefficient
Cz Local or complete-wing lift coefficient
f C, locoL
l CL =
4
'rESTS WITH THREE-DIMENSIONAL ADJUSTMENTS IN THE RECTANGULAR WORKING SECTION OF THE FRENCH T2 WIND TUNNEL, WITH AN
AS 07-TYPE SWEPT-BACK WING MODEL
A. Blanchard, M. J. Payry, J. F. Breil
1 ... INTRODUCTION
This test series follows a study done in the T2 wind tunnel
with the goal of defining a shape for the adaptable walls which
would minimize their influence on three-dimensional objects
placed in the center of the section or fastened on the side.
The present configuration of the working section does not
allow obtaining a shape identical to that of the layer of
current existing around a three-dimensional model in unlimited
atmosphere (two completely rectilinear and parallel lateral
walls, two flexible and bendable upper and lower walls). The
planned solution thus consists of using the two bendable walls
to minimize the influence of the walls on the model.
The method implemented uses solutions developed by "E.
Wedemeyer and L. Lamarche" [5]. A first series of tests was
done in cooperation with the University of Berlin on various
existing models [6]:
- a C5 revolving body 166 mm long, 0.3% blockage;
- a civil F4 airplane model with 120-mm wingspan and three-
component balance;
- a duck-type military airplane model with the same balance.
Another series of tests was then done on a bigger model [7]:
- a C5 body 400 mm long, 1.8% blockage.
*Numbers; in the margin indicate pagination in the foreign text.
5
The results and calculations were compared.
The calculation method was optimized for revolving bodies
placed in the center of the section; an extrapolation was tried
which placed a half-wing at the wall. In this case, calculation
is done as if the section were twice its actual width, using the
Mach distribution at the wall measured near the plane of
symmetry.
The results obtained on the "16/1000-scale" AS 07 are
discussed in this report. They can be divided into two groups:
control tests and systematic tests.
Included in the first group is control of wing angling by
rotating the walls. The path of the jacks would not permit the
displacements required by calculation for angling the model to
+2·; we thus used this artifidial method after having verified
its validity.
The three-dimensional adaptation method supplies the
optimal shape of the walls from the first calculation, whatever
the initial position of the walls; this was verified in 18 several test configurations. Finally, an adaptation called
"two-dimensional" was tested; it uses the normal method for T2
profile tests. This case, without theoretical justification,
was tried to see the influence of the shape of the walls and the
size of errors which can be made.
The second part of this study corresponds to systematic
tE~StS: four configurations were chosen which gave different
lift coefficients, without making highly supersonic zones appear
on the profiles. For each configuration, three wall positions
were tested:
- The first, called "unadapted," corresponds to the upper
and lower divergent rectilinear walls compensating for
6
thickening of the limit layers; it served as our basis
for beginning three-dimensional adaptation calculations.
These particularly simple limit conditions can also be
used for complete calculation of the flow in the working
section.
- The second wall shape comes from the three-dimensional
adaptation calculation; the flexible sheets are
positioned before the gust.
- Finally, the last case corresponds to "two-dimensional'
adaptation"; the iterative process converges on a single
gust.
For each type of test, three gusts are necessary to obtain
readings from the six rows of pressure recorders spread along
the AS 07 wing.
The experimental results gathered during this series are not: sufficient to validate the three-dimensional adaptation
method used. Additional calculations must be made to estimate
residual corrections. In these tests, a negligible influence of
the walls is observed for low lift values or low Mach numbers;
inversely, for 2 degrees of incidence or for Mach 0.8, the gaps
become significant and can in part be interpreted as variations
in aerodynamic incidence.
2 - ADAPTATION PRINCIPLE
The purpose of the adaptable walls is to create an
unlimited flow around a model in a working section with finite
dimensions; this can be done by controlling the wall conditions,
either by their shape in the case of solid walls or by flows of
mass through porous walls. The first solution has been chosen
at T2, where flexible sheets moved by jacks form the upper and
lower plates of the working section [3].
7
In the case of a three-dimensional body, it is necessary to
bend the walls located around the model to arrive at a shape
near the layer of current existing around the model in unlimited
atmosphere. This solution is not at present possible at T2, but
on the other hand it is possible to use the two flexible /9
walls to minimize residual corrections due to the influence of
the walls on the object.
2.1 Two-dimensional adaptation
The details of the process will be found in [2] and
[4]; it uses a coupling between the real flow in the working
section (internal field) and a calculated virtual flow outside
the wind tunnel (external field). Coupling occurs on a control
surface near the walls through speed vector components.
Adaptation is achieved by an iterative process acting on the
shape of the walls: the components of the speed on the control
surface become available at each iteration; they are
extrapolated from the pressure measurements at the wall. The
velocities needed on the control surface to achieve an unlimited
external flow are calculated by the Green function following an
inverse method. A method of optimized relaxation between the
internal and external flows for the vertical velocity component,
followed by an integration along each flexible wall, supplies
the new shape of the wall. The real shape needed is obtained by
adding the thickness displacement of the four wall limit layers.
2.2 Three-dimensional adaptation
For three-dimensional adaptation, the process is
different [5]: it uses schematization of the model through
distribution of sources and vortices in a narrow horseshoe
placed on the section axis. This schematization gives a good
representation of axis ymmetrica 1 bodies mounted in the middle of
the working section.
8
The originality of the method lies in then doing a
linear transformation, which permits passing directly from
distribution of velocities at the walls to the adapted form
without needing to determine the intensity of singularities.
The optimized shape of the walls is thus theoretically obtained
from the first calculation; this shape, which is not exactly
"adapted," minimizes residual corrections on the model caused by
the influence of the walls.
Using this method for a half-wing at the wall is
abusive, because the base schematization does not represent a
wingspanJ it has nonetheless been tried here by replacing the
lateral door by a plane of symmetry leading to a fictional
double section width, and taking the Mach distribution of the
flexible walls near the plane of symmetry as reference.
3 '- EXPERIMENTAL EQUIPMEN'I'
The T2 transonic wind tunnel is pressurizable and can
function at low temperaturesJ only minimum-pressure and ambient
temperature tests were done during this series.
3.1 Working section equipment
The working section has an almost square section of
0.39 x 0.37 mm 2 at the entrance. Flexible sheets of Invar
make up the upper and lower walls, equipped with three rows of
pr.essur4~ recorders whose coordinates are given in figures 7 and
8. The sheet-positioning mechanism is described in [2], [3],
and [4].
The left lateral door has three portholes with
pressure recorders placed along horizontal and vertical lines
whose coordinates are shown in figures 7 and 9.
9
The pressure recorders are linked to the Scanivalves,
each of whose head can observe 48 positions in 5 seconds.
The position of the wing in the working section is
given in figure 6.
The Mach number of the flow is set by a second neck
controlled by the computer which controls the gust.
No other equipment or wind tunnel measurement method
was used.
3.2 Mounting the win~
The AS 07 wing model with a scale of "16/1000" is
shown by the photographs in figure 5. The method of mounting
the wing on the wall is shown (figure 6), the plane of the wing
and its specifications are given (figures 10 and 11), and the
shape of the profiles which compose it and the positions of the
pressure recorders are indicated (figures 12 and 13).
There are six rows, each with 16 recorders on the
inner and outer sections and one on the leading edge; they are
placed across the wingspan so as to form lines with constant
chord percentages. These recorders communicate with tubes
placed in grooves along the wingspan; each tube communicates
with three recorders (either on the external wing or on the
internal wing). When one of the three rows of recorders is used
to measure pressure, the other two are covered with thin (0.05-
mm) adhesive strips. It is thus possible to simultaneously
measure pressure on two sections of the wing (one internal and
one external); measurement of velocities over the entire wing
thus requires three different gusts.
The wing is mounted on a half-fuselage linked to a
porthole, whose rotation ensures the angling of the wing-
10
fuselage assembly; the angular reference is the rectilinear part
on the back of the fuselage [1].
3.3 Acquisition and examination program
The T2 wind tunnel is linked to a team of two
computers, one concerned with creating and regulating the gust
and the other with obtaining data and storing measurements to
disk at the end of the gust.
These tests are pursuant to the series done on the /11
C5 body and use its principal elements.
Disk car.~:ridge LU 26, Program
LU 34, Test files, calculation files
AC9uisit:Jon program
(TEACQ)
(RAFAL)L PARe 5
or
PARC S
(lance ACQC5)
(uses PROJ and ADAP.)
Fixed walls:
No adaptation
during gust
Two-dimensional
adaptation
Initialization of programs {With (TR,) RINC 5 (For PARC 5)
or (TR,) RINC S (For PARC S)
Test file
AD --- test number from AD 100 to AD 173
11
Wall posJ tioning file
- any test file AD---
- or calculation file AD 9 -._-
- or'special file AD 4: Divergent rectilinear walls of
symmetrical limit layers.
AD 444: AD 4 + 10' rotation upward
AD 445: AD 4 + 30' rotation upward
ThFee-dimensional adaptation calculation
Calculation from a test file AD
VKJ 43 Calculation of wall shapes without rotation
VKI M Calculation of wall shapes with rotation
LD
I ')J::=:=--I
~ - - - ---- - - - - - -. 780 "''''
---tFiling to disk
... J
I
:h:370 mm
, Of
- section length 780 mm
- ratio c = h/b = 2.1081
- reference recorders:
right lateral RL
weighting coefficients
file VKJ - R (cartridge
LU 43)
File for new calculated wall shapes
AD 9 --- beginning test number for the calculation
grograms for examination of AD--- files
l,TCS:
- graphs local profile Mach numbers
- graphs Kp
- lists AD file
- calculates Cz
12
LTC 51:
- graphs wall Mach numbers
- graphs wall shapes
starts LTC 52 (does an RP, LTC 52)
LTC VK:
- graphs only wall shapes calculated by VKI 43 or VKIM
(from AD 9---).
4 - SUMMARY OF TESTS PERFORMED
A previous study was done on the AS 07 wing [11. We
verified in one case that the same results would occur, although
the working section was modified when the T2 wind tunnel was
adapted for cryogenics.
The first control tests were done by measuring rows 2 and 5
of pressure recorders for the Mach numbers and incidences
indicated below:
Mo J 0,6 0,7 0,8 )
0( -) ( )
( +20 X X X )
( 0 x x x )
( _2 0 X X )
( )
13
Four configurations WE!re selected for systematic tests: /13
)
0,6 0,7 0,8)
--~~--~~--~--~~ x )
( ::) (--- ---:--:----)
(0° X: : X ) ( ::) (------- ------- -------:-------) (~2° X ) ( )
They correspond to a sampling of lift coefficients and to an
infinite Mach effect upstream, while limiting the supersonic
zones which appear on the profiles.
Figure 1 shows the list of tests in chronological order,
and figures 2, 3, and 4 classify them by configuration.
We first showed that rotation of the upper and lower walls
was equivalent to angling the model at the same angle. This
artifice was made necessary because the path of the jacks did
not permit the displacements required by calculation of
three-dimensional adaptation for a model incidence of +2-_
- Divergent rectilinear walls
·Mo ( )
I:l( ,( 0( _ ~~~I_ J 0, 6 0, 8 ) Ihf.naJ.. ( D\$ elAJ ,,"l1}..lU' )
( ) +20 ( +2° AD 4 AD 120 )
( +1,5° AD 445 AD 122 ) ( :) (----------- ----------_.-: -------------)
O· (0° AD 4 AD 107 - AD 109 AD 108 - AD 132 ) ( -0,5° AD 445 AD 137 AD 139 ) ( )
14
- Three-dimensional adapted walls
Mo
( )
( 0( CALCUL 0,6 0,8 )
0( aerod •• 0° ( ) (-- ) ( 0° VKI 43 117 AD 119 ) ( -0,5" VKI M 138 AD 141 ) ( )
The three-dimensional adaptation method theoretically
supplies the optimal shape of the walls from the first
calculation, whatever the initial position of the flexible
sheets. Controls were done in this respect for the following
configurations:
Mo ( ) ( .cl..
J. 0,7 0,8)
( .~p .. " ) ( ) ( +1,5° AD 127 (I) ) ( AD 128 (2) ) ( : AD 129 (3) )
(-------- ----------: ---------) ( :) ( 0° AD 115 (I) : AD 118 (I) ) ( AD 116 (2) : AD 119 (2) ) ( : .. ) (----- -------: --- ----)
( -0 , 5 ° AD 1 40 (I) ) ( AD 141 (2) ) ( : . )
The figure in parentheses after the file number indicates the
order of the iterationJ the wall-positioning file thus results
from calculation of the preceding test. (Iteration (0) is the
test done with rectilinear walls.)
/14
We also verified that the tests called "two-dimensional
adaptation" converged rapidly, as is the case for the profile
tests; it is sufficient for that to compare the wall position of
15
the 3rd and 4th iterations done during the same gust; the two
positions are always close. In general, the beginning shape
chosen is near the adapted shape, but we have tested this
convergence in the two particular cases when the beginning shape
was far from the adapted shape. The beginning file chosen was
AD 4: rectilinear walls divergent from limit layers and
symmetrical.
Configuration: Mo = 0.7 ~ = +1.5·
Configuration: Mo = 0.8 ~ = o· File AD 130 (1)
File AD 133 (1)
followed by File AD 134 (2)
Comparisons were made between the various wall positions;
they are noted:
- "Non," for divergent rectilinear walls
- "2D," for two-dimensional adaptation done with the PARCS
program - "3d," for positioning of the walls in the shape
calculated by the VKI 43 or VKI M program
It was decided to do systematic tests for the three cases
of "adaptation," the non-adapted case serving as a basis for
three-dimensional calculation (any wall shape will work); this
case can also serve as a basis for complete flow calculations,
because here the limit conditions are particularly simple. The
two-dimensional adaptation, a priori outside the subject of the
study, was systematically tested to use as a comparison with the
assumed optimal shape.
Finci11y, four configurations for three cases of adaptation,
reproduced three times to have the velocity field on all of the
wing, were tested; these 36 gusts make up the systematic tests
listed in figure 26a.
16
5 '. CONTROL TESTS
We will not present all the tests done, but only a
selection of cases judged most interesting, since the goal of
this series is not to evaluate the AS 07 wing.
5.1 Angling by wall rotation
Of the five configurations tested (paragraph 4), three
are presented. The first corresponds to Mo = 0.6 and ~ = +2·
for rectilinear walls (figure 14); this is the configuration
which obliged us to use this artifice, as the three-dimensional
case could not be tested.
Figure 15 shows the comparison of Mach numbers on the
walls and on the wing, for an aerodynamic incidence equal to o· and a Mach number equal to 0.8, in the case of rectilinear
walls. Figure 16 presents the same configurations but for wall
shapes coming respectively from calculations VKI 43 and VKI M.
The results of figures 14 and 15 show that the high
Mach case is the most recordable, but the correspondence of the
tests remains good. Figure 16 shows that the VKI M calculation
makes perfect allowance for total rotation.
It is thus possible to display a model incidence /16
different from that desired and to compensate by rotating the
walls.
5.2 Convergences of iterations
5.2.1 Three-dimensional adaptation
Several calculations for optimization of wall
shape were connected for one configuration. The last test is
always recalculated, leading to a wall shape which by definition
17
will not be used, but which will in fact constitute an
additional iteration.
Of the four tested cases, two are presented in
figures 17 and 18; the first (Mo = 0.7 and = 0·) shows that
the adapted shape is practically obtained from the first
iteration; in the second case--much more difficult (Mo = 0.8
and « = +2°)--it is necessary to wait for the second
calculation. This second case corresponds to a freely
supersonic regime of the wing which will not be studied
systematically herein.
5.2.2 Two-dimensional adaptation
In all tests done, the 3rd iteration is always
identical to the 4th and last iteration of the gust, even when
the upper and lower walls have been prepositioned in a shape
very different from the "adapted" shape. This is the case shown
in figure 19 corresponding to Mo = 0.8 and oc = 0·.
To confirm the validity of this statement, a
second test was done, positioning the flexible sheets on the
preceding shape; the values obtained can thus be considered to
correspond to the 4th, 5th p 6th, and 7th iterations of the test;
they are all identical (figure 20), which confirms that the
convergence was well obtained.
5.3 Non/2-D/3-D comparison
Two cases are presented here, one of which is not part
of the systematic tests:
- Mo = 0.7
- Mo = 0.8
18
The gaps observed following the types of "adaptation"
will become more significant as lift and Mach number upstream
increase. The adaptation called "two-dimensional" gives results
nearer to the non-adapted case; in fact, everything happens as
if the aerodynamic incidence of the two-dimensional case were
higher than that of the tests with a wall shape adapted in three
dimensions. On the other hand, rectilinear walls lead to a
higher effective Mach number upstream (blockage effect).
In the first case (figure 21), the gaps are moderate;
they are more significant in the second case (figure 22).
Observation of the direction of the walls leaving the convergent
(figure 21) shows that effectively the direction of the flow
upstream is no longer horizontal in the "2-D" case, unlike the
"3-D" case; the angular reference was given by the "non-adapted"
case. The effect produced is incontestable, because we /17
previously demonstrated that rotation of the wall assembly
modified the aerodynamic incidence of the model; however, this
is not sufficient to prove that the 2-D case is erroneous,
because the direction of the current lines in unlimited
atmosphere is not known. We note also the very different shapes
of the walls downstream; they go downward for the "3-D" cases,
which is logical allowing for the chosen schematization
(horseshoe vortex) and the calculation made (in the plane of
symmetry). But once more, that does not prove that the shape
obtained is optimum.
Finally, one can observe on the last figure (23) that
the effect produced by modifying the shape of the walls is not
constant across the wingspan. This was predictable due to the
working section geometry itself, allowing for twist of the wing
and for three-dimensional effects.
19
5.4 Visualizations
For three configurations, oil visualizations were done
on the left door of the working section, giving the direction of
the current lines 55.4 mm from the end of the wing. Reference
marks were made, making it possible to locate the positions
relative to the current lines and to measure their deviations.
W~Q..k"I\'lI -:.e(.~, .. 1')
Av.16
• &()o ... ~()o .200 - Zoo . -+. -. _ .. _.--. -·1--· -._.
I
The end of the wing is located between the abscissas
91.06 mm and 135.86 mm from the porthole (figure 6) and very
near to the section axis (function of the incidence).
The maximum deviations noticed are located on the
section axis slightly behind the tip of the wing (figures 24,
25, and 26).
( Walls dmax ) ( MQ 0( ) ( ) (
"Non-adapted"; )
Figure ( 0,6 +2° (S° •..•.. 6°) ) ( AD 4 ) ( -- - .:-------) ( ) ( 0,6 +2° · (S° ...... 6°) ) ( 'Adapted 2-D: ) Figure · . ( : --- -:-------) (---:--- · ) · ( 0,6 _2° "Non-adapted": "0,5- ) Figure ( ) ( AD 4 )
24
25
26
20
The photos taken from behind clearly show the /18
deviations of the current lines.
6 - SYSTEMATIC TESTS
For the 36 gusts that made up the systematic tests
(paragraph 4 and figure 26a), the following information is
given: wall shape (figures 27 and 28), Mach numbers of the
three rows of recorders on the adaptable walls (figures 29, 30,
31 u and 32), Mach numbers of the left lateral door (figures 33,
346 35, and 36) following the horizontal axis or the three
verticals, and finally spread of Kp on the AS 07 wing (figures
37 to 44).
Numerical values for these curves are given in the attached
test listings. File numbers corresponding in chronological
order to the experiments were kept in the interests of clarity.
Here will be found a systematic comparison of the three
cases of adaptation--"Non/2-D/3-D"--and their influence on the
speed distributions whose principal characteristics were seen in
paragraph 5.3.
Finally, integration of Kp for each section supplies local
lift coefficient Cz. The values are tabulated in figure 45;
they were traced along the wingspan of the various
configurations tested (figures 46 and 47). It is observed that
the internal wing changes less rapidly than the external wing
with incidence (figure 46) or Mach number upstream (figure 47).
On the other hand, the gap between the "non-adapted" and
"adapted 3-D" cases increases with the lift.
21
Local Cz were multiplied by the chord of the profile in the
section considered; the product Cz • C represents local /19
contribution to wing lift. The values obtained were traced in
this representation (figures 48 and 49); this weighting mOdifies
the appearance of the curves ("elliptic" distribution plane),
but the observed tendencies are the same.
Finally, integration of the curves in this last
representation supplies the overall lift coefficient of the
wing, which was reported as a function of incidence (figure
50). We have also reported the lift measured during the
preceding series [1], done between rectilinear walls for a Mach
number upstream of 0.47. The effect of compressibility is felt
more as supersonic zones develop on the wing.
7 - CONCLUSION
This series of tests on the AS 07 wing is registered as a
study on three-dimensional adaptation of the T2 wind tunnel. It
uses the two flexible walls to minimize residual corrections in
the presence of a three-dimensional model. It implements the
"E. Wedemeyer and L. Lamarche" method where schematization of
the model by a distribution of singularities adequately
represents an axisymmetrical body. Extrapolation of these
methods in the case of a half-wing at the wall has no ultimate
goal; it serves merely as a preliminary phase, to observe the
influence of wall shape in various sections of the wing, to
study the convergence of the method, and to make adjustments
(rotation of walls, incidence, etc.,.
On the other hand, these experiments can serve as a basis
for calculating potential three-dimensional flow around the
model. Then, a three-dimensional object placed in the section
22
could be more elaborately schematicized; it would lead to
development, as for axisymmetrical bodies, of a method of
adaptation minimizing the influence of the walls on the model.
At present, it is difficult to know if the shape called
"adapted 3-D" is nearer to the values of unlimited atmosphere
than the shape "adapted 2-D," but it is definitely not the
optimum shape.
The tests will next be completed by directional limit layer
readings on the lateral wall at the level of the end of the
wing. The direction of the current lines in this area will be
an important element in the reality-calculation comparison.
23
REFERENCES
1. A. Mignosi, A. Seraudie. "Etude d'une maquette d'aile en fleche a la soufflerie T2 de l'ONERA-CERT [Study of a swept.-back wing model in the ONERA-CERT's T2 wind tunnel]." DE RAT technical note No. 13/5006 ON, March 1977.
2. J. P. Archambaud, J. P. Chevallier. "Utilisation de parois adaptables pour les essais en courant plan rUse of adaptable walls for tests in plane current]." ONERA TP No. 1982-3B, AGARD/FDP meeting in London, May 19-·20, 1982.
3. J. P. Archambaud, A. Seraudie. "Etudes de parois adaptables a T2 [Adaptable wall studies at T2]." ONERA TP NO. 1983-150, 20th AAAF Colloquium, Toulouse, November 8-10, 1983.
4. J. P. Chevallier, A. Mignosi, J. P. Archambaud, A. Seraudie. "Adaptable walls in the T2 wind tunnel: Principles, execution, and some examples of two-dimensional results." La Recherche A~rospatiale, 1983-4, pp. 217-235.
5. L. Lamarche, E. Wedemeyer. "Minimization of wall interference for three-dimensional models with two-dimensional wall adaptation." V.K.!. Technical note 149, Rhode Saint Genese, Belgium, March 1984.
6. J. P. Archambaud, J. B. Oor, A. Mignosi, L. Lamarche. Premiers essais d'adaptation des parois auto-adaptables bidE~msionnelles de la soufflerie T2 autour d'obstacles tridimensionnels [First. adaptation tests of two-dimensional self-adapting walls at the T2 wind tunnel around threedimensional obstacles]. OA Technical Report No. 33/3075 (DERAT 11/5015 DN), September 1985.
7. J. P. Archambaud, J. B. Dor, M. J. Payry. Rapport sur la deuxieme campagne du C5 [Report on the second C5 series]. (TO be published soon.)
24
LIST OF FIGURES
1. Test tables
- List of tests - Rows of recorders 1-4 - Rows of recorders 2-5 - Rows of recorders 3-6
2. Mounting the wing in the section
Figure
1 2 3 4
- Presentation of mounting 5 - Drawing of wing mounting 6 - Drawing of pressure recorders on walls 7 - Pressure recorder specifications - flexible walls 8 - Pressure recorder specifications - lateral portholes 9 - Plane of the wing 10 - Dimensions of the wing 11 - Profiles 12
Specifications of wing pressure recorders 13
3. Control tests
3.1 Rotation
- First control (~= +2·, Mo = 0.6 Non-adaptable) Wall shape Wall Mach Profile Mach
SE!cond control (r/.. = 0·, Mo = 0.8 Non-adaptable) Wall shape Wall Mach Profile Mach
Third control (0( = 0·, Mo = 0.8 3-D) Wall shape Wall Mach Profile Mach
3.2 Convergence of iterations
a .. 3-D
First case (0£= 0·, Mo = 0.7) Wall shape Profile Mach
Second case (ol= +2·, Mo = 0.8) Wall shape Profile Mach
14
15
16
17
18
25
b - 2 - D (0( = a ., Mo = o. 8 )
- Beginning of AD 4 (File AD 133) Wall shape Profile Mach
- Beginning of a similar shape: AD 133 (File AD 134) Wall shape
19
Profile Mach 20
3.3 Non/2-D/3-D comparison
- ( 0( = o· , Mo = 0.7) Wall shape Wall Mach 21
- (0<. = o· , Mo = 0.7) Profile Mach (2 ) Profile Mach (3 ) 21
- co(. = o· , Mo = 0.8) Wall shape Wall Mach 22
- (I>( = 0·, Mo = 0.8) Profile Mach (2) Profile Mach ( 3) 22
- (0(, = a·, Mo = 0.8) Kp 23
4. Visualization, left lateral door
- (O( = +2· , Mo = 0.6) Non - front Visu (2 ) - back 24
- (ex = +2·, Mo = 0.6) 2-D - front Visu ( 1) - back 25
- ( CI{ = +2· , Mo = 0.6) Non - front Visu (3) - back 26
5. Use in 4 base cases
5.1 Wall shaEe
-tol = -2· Mo = 0.6 _ot = +2· Mo = 0.6 27
-c:( = O· Mo = 0.6 -0( = O· Mo = 0.8 28
5.2 AdaEtable wall Mach
- (fI... = - 2 • Mo = O. 6 ) - Non - 2-D - 3-D 29
26
- (01. = o· Mo = 0.6) - Non - 2-D - 3-D 30
- (~ = +2· Mo = 0.6) - Non - 2-D - 3-D 31
- (~ = o· Mo = 0.8) - Non - 2-D - 3-D 32
5.3 Lateral wall Mach
- (Qt. = -2· Mo = 0.6) - Non - 2-D - 3-D 33
- (0£ = o • Mo = 0.6) - Non - 2-D - 3-D 34
- (0/. = +2· Mo = 0.6) - Non - 2-D - 3-D 35
- (oot = o· Mo = 0.8) - Non - 2-D - 3-D 36
5.4 !S£
- (cit = -2· Mo = 0.6) Non adaptable 37
- (cit = -2· Mo = 0.6) - Non - 2-D - 3-D 38
- «(:0( = O· Mo = 0.6) Non adaptable 39
- (c>( = o· Mo = 0.6) - Non - 2-D - 3-D 40
- ('coI. = +2· Mo = 0.6) Non adaptable 41
- (IOJI-= +2· Mo = 0.6) - Non - 2-D - 3-D 42
- (lOt. = o· Mo = 0.8) Non adaptable 43
27
- (0(.= o· Mo = 0.8) - Non - 2-D - 3-D
5.5 Cz
- Cz recapitulative - Cz Mo = 0.6 (3 inc.) - Cz Cot = O· (2 Mach) - Cz X chord Mo = 0.6 (3 inc.) - Cz X chord 0(. = O· (2 Mach) - Cz (oc.)
44
45 46 47 48 49 50
28
TEST TABLES
FIGURES 1 TO 4
29
Figure I
List of "AS 07 wing" tests
File AD4 Divergent ~li·ne·c1'r- walls AD445 · · Idem + 30' rotation (upward) AD--- · · Test file No. ---AD9---- · · 3-D calculation of new wall position
A File ?> c... v £
~ Rows of Recorders
*~*~~~***.**.~~~~*~~4*~~**~~**~~~~~~~~~*~ •• ~.*~**~*~*~~*.~~~~. "A 'HIC.' PFI~IGEES 'FICHtER ROT.' 'riB. i+ "F t ,:H I ER 'AFF. '~lACH DE PR t '~e::~ 'DE DEPART PARa I:3' ADAPT.' D' I TE? .. ~.~~****!**~*f~*~~ ~~~~*~*~~!~~~~.~.*; **;*~*!~~~*~~*!~~~~~~~~ ,.. AD 1 a~' a, .;' z. - ~ 'AD4 .a, NO~I , 1 ,;
c..Starting File
D Wall Rot.
E No. of iter.
" AD 1 07 .a .6 a 1 ;;. ;,; FtD10S 13 .:3 13 1 ,; ;;. AD11a -2 • (' a , .. , 1 It
,; AD11~ .a • (' AD'?la~.) '3-D 0)' 1 " ,; AD111i a ., AD'311~ 133-0 CZ" 1 ,; ,. ADlli' a .6 I1D':la7 a 3-D' 1 ,; ,; AD113 a .8 AD9108 a 3-D (1)' 1 ;,; ;or ADll'~ .) .:3 A0911S a :3-D (~;. 1 ,. "" AD lZ.a , +;2 , • .; AD4 a rlO~1 1;r * AD122 ,+1." • 6 ADH~ 313' NON 1 It
* AD123 '+1. 5' .6 I1D9122 30' '3-0 1" * AD124 '+1.5' •• A044~ 30' NO~I 1'" * AD12~ '+1.~ .7 AD9t;N 30'3-0 1;;. ,; AD 126 ,+ 1. 5 .3 AD44'5 :313' ~IOrl 1,; '" AD12? '+1. S .:3 AD9126 :313' ]-0 (1;' 1 ". ;or AD129 '+1.5 .:3 AD'?12(, 313' '3-D (2) 1 .. ;;. AD129 ! "'1. ~ .:3 AD9123 30'3-D (3)' 1 ". ;;. AD130 '+1.~ .7 AD4 a 2-D 4,. " AD131 ''''1.~ .6 I1D13.) 0 2-D 4,. ,. AD133 a .:3 AD4 a 2-D 4,. ;;. AD134 a .:3 AD133 a 2-D 4 .. ,. AD13~ a •• AD134 a 2-D 4 * ;;. AD13f:i .a .6 AOll5 a 2-D 4,; ;;. AD137 '-0. S .6 ADHS :313' rlQH 1 * ... AD138 !-.).~ .6 AD'?137 30' 3-D 1 "" ;;. AD13'3 '-0.5 .:3 ADH~ 30' t~ON 1 "" ;;. AD14a !-a.s .:3 AD':13', 313'3-0 (1) 1 ,.. ;,; I1D141 '-0.~, .:3 A0914.) 313' ,'3-0 (2) 1 .. ;;. AD 142 ! -2 .';' AD4 a! tNH 1 ... '" AD143 ! -2 , • .; AD9142 a :3-D 1'" ,. AD144 ! -2 ! .6 1101:36.) 2-0 4,.. .. AD14~ ! +2 ! .6 A0131 a! 2-D , 4 "" ~-------!----!---- ---------!--------- ~-----!-------!-------~ ;;. AD141.i ! +2 ! • Ii 4! AD1 .. 5 0 2-D 4;; ;; AD147 !",1. '5! • Ii A044~ 30' HON 1 + ~ ADI4:3 '+1. ~, .Ii AO?122 30' :3-D 1 .. ;; A014'3' 0! • .; AD136 \) 2-D 4,. ;; ~Dl~0! 0! .6 At!4 0 tlON 1,; " AD1~1 0 • .; AD91a7 ~ 3-D 1" ;; AD1~Z 0 .3 A0134 0 2-0 4;; ;; AD1~3 a .:3 • A04 a rh)N 1" ;; A01~4 .) .:3 AD': 11:3 a 3-D 1" ;;. A01~' -2 .6 AD144 a 2-D 4;; '" A.Dl''; -2 • Ii A04 0 NON 1" ~ AD1~7 -2 .6' AD'314~ 133-0 1" ~-------!----!----~---------!-------_-I------!-------! _______ ~ '+ AD1~a -2!.';!3 - 6 I AD144 ! ~ ! 2-D ! 4 '" '" AD1", -2 .Ii A04 , 0 'NON 1;; ;;. A0160 -2 .Ii AD':142 133-0 1'" ... A0161 a • Ii AD131.i 0 2-D 4" .. AO 1 f:i2 a • Ii AD4 a NON 1 .. ;;. A0163 a • Ii AD':1137 0 3-0 1;; ... ~Ul1i4 0 .8 AD134 0 2-D 4'" ... AD16~ \) .:3 AD4 a rl')N 1 '" .., ADI6'; a .8 A09118 a 3-D 1 .. ,.. A0167 +1.5! .6 A044'5 :313' NON 1;,; ;,; A016:3 +1. S! • .; AO',122 30'3-0 1 '" ,.. AD16'; +2'.'; AD1"'5;a 2-D 4" ~~~~*.+~ ~~~~*~~~~~~*~~~~~~~~*~~~~~~~~~~~+.~~~~~~~+.~~~~~~~~~~~~
30
Figure 2
Rows of recorders 1-4
r--------------------------------------------------, I NON ADA PTE I
~--------------------------T-----------------------~ I Incidence I Mach I
~----------~---------------+-------~-------T-------~ I AfHchee I Aerodynanlique I 0.6 I 0.' I 0.8 I
~----------+--------------- ~ I I +1.5 I +2 14' I I
~----------+--------------- -------+-------+-------I 0 I 0 150 I I 153
~----------+--------------- -------+-------+-------I -2 I -2 156 I I l __________ ..1 __________ • _____ "-___ ... ~L.. ____ ~ ___ -'
r--------------------------------------------------, F~OAPTE 3-~
~--------------------------T-----------------------~ I Incidence I Mach I
~----------~---------------+-------T-------T-------4 I Affichee I Aerodynamique I 0.6 I 0.' I 0.8 I ~----------+--------- .. -----+_---~---__t---_I I +1.5 I +2 148 I I
~----------+--------------- -------+-------+-------I a I 0 151 I I 154
~----------+--------------- -------+-------+-------I -2 I -2 15' I I L __________ ..1 _________ •• _____ ...... ___ --li. ____ -"-___ --'
r--------------------------------------------------, I AOAPTE 2-D I
~--------------·-----------T----~------------------4 I Incidence I Mach I
~----------~---------------+-------~-------T-------~ I AfHchee I Aerod~:'"atnique I 0.6 I 0.' I 0.8 I ~-.---------+---------.------+_---+----+_--___t I +2 I 146 I I
~----------+--------------- -------+-------+-------I 0 I 149 I I 152
~----------+--------------- --- ..... --4-.... ---.---+-------155 I -2 I I I l .. _________ J _________ . ____________ .L ____ .... ' ___ --'
Affichee - Displayed
31
Figure 3
Rows of recorders 2-5
r--------------------------------------------------, I NON ADAPT! I
~--------------------------T-----------------------~ I Incidence I Mach I
•. ----------'T-~-------·-·----':"+-------·r-------'T-------~ I Affichee I Aerodynamique I 0.6 I O.? I 0.8 I I. __________ +---------·-·-----?-----JI-----+-'----t I I +2.17 121 I I
I ·2 ~--------------- -------.-------+-------I I +2 120 I 1
~----------+--------------- -------+-------+-------I +1.5 I +2 122 I 124 1 126
~----------+--------------- -------+-------+-------I 0 1 0 10?' I 105 I 109 I I 109 I I 132
~----------.--------------- -------.-------.-------I -0.5 I 0 13?' I I 13~
~----------+--------------- -------+-------+-------I -2 I -2 142 I 110 I L __________ .L ________ • _______ ~ ___ .01.' ___ .....1 ...... __ .....1
r--------------------------------------------------------, I ADAPT! 3-D I
~--------------------------'T-----------------------------4 I Incidence I Mach I
.----------'T---~--------~--+-------T----------T----------~ I Affichee I Aerodynamique I 0.6 I a.?' I 0.8 I • __________ +---------------LL I I 12?,(1) I +1.5 I +2 123 125 128(2) I I 1 I 129(3)
.----------+--------------- -------+----~-----+----------I Q lOll?' 1 115(1) I 118(1) I 1 I 116(2) I 119(2)
~----------+--------------- -------+----------+----------I - 0 .5 I 0 138 1 I 140 ( 1) 1 1 1 I 141(2)
.----------+--------------- -------+--------~-+----------1 - 2 1 - 2 143 1 I l-~---- ____ J. _____________ • __ ....... ___ _:lIIoo...----..... -----..J
r--------------------------------------------------, I ADAPT! 2-D I
.--------------------------T-----------------------~ I Inc idence 1 Mach I
.----------T----------~----+-------'T-------'T-------~ I AF Fichee I Aerodyrlamique I 0 .6 I 0 .?' I 0 .8 I • __________ +_______________L I +2 I . 145 I I
.----------+--------------- -------+-------+-------I +1.5 I 131 I 130 1
.----------+--------------- -------+-------+-------,I 0 I 136 1 135 1 134 .----------+-------_._._----- ------.-+-----~-+-------1 -2 1 144 1 I l __________ J_______________ I
32
Rows of recorders . . 3-6
r--------------------------------------------------, I NON ~D~PTE I ~-----------------------·--T-----------------------4 i Incidence I Mach I
~----------T----------··----+-------T-------T-------~ I Affichee I AerodynamiqQe I 0.6 I 0.' I 0.9 I ~---------- ~-- --------.. ----+----I-----f----i I +1.5 I +2 16' I I
.----------+--------------- -------~-------+-------I a I 0 162 I I 165
.----------+--------------- -------+-------+-------I -2 I -2 159 I I L __________ ..l __________ •• ____ .-____ .. ____ ~I ___ _'
r--------------------------------------------------, I . ADAPTE 3-~ I
~--------------------------T-----------------------4 I Incidence I Mach I
~----------T--p------------+-------T-------T-------4 I Af fichee I Aerod~n~LmiqQe I a .6 I 0 ., I 0 .8 I ~-- ___ -- ___ I _______ - .. ___ -- _ +-____ ',.11-___ +-___ -; I +1.5 I +2 168 I I
~----------+--------------- -------+-------+-------I 0 I 0 163 I I 166
~----------+--------------- -------+-------+-------I -2 I -2 160 I I I. __________ J. ________ •• ______ ....... ___ .... I ___ ---i"--__ ~
r--------------------------------------------------, I AD~PTE 2-D I
.--------------------------T-----------------------4 I Incidence I Mach I
.----------T---------------I-------T-------T-------4 ~ Affichee I AerodynamiqQe I 0.6 I 0.' I 0.9 I !~----------+--------.-------+_----_f'------...._I---._; I +2 I 169 I I
~----------~--------------- -------+-------+-------I 0 I 161 I I 164
.----------+--------------- -------+-------+-------I -2 I 158 I 1 L __________ ..l ________ . _______ .-. ___ ... ' ____ ..... ' __ ___
Affichee = Displayed
Figure 4
33
Figure 5
Presentation of mounting
34
WING MOUNTING
FIGURES 5 TO 13
35
w
""
~~~"",,,~~,>;»» > "----------f-------..... > '> '> i> :> '> I , ... - __ - ___ _
x
y
~
----.,----
Wall ref. j
w W .f'-
7 > 7 7 7 7 7 7 7 7 17 7 7 7 7 7 7 7 777 7 7 7 717 7~ c
~
ro Diagram of wing mounting
""
W --..J
'.L..-
v ~
I
--- -31 31 • " 'l ~ 'I 'J t'ia;;;'!fJ~ft'" " .a f4 " tr. -~ .. _- --4-- i6 e- • I .. - .. e -
n 3l 31 2lt7 III U 11 11 i7 t, ij tJ' H!!:H 1'1 iI f2 i4 i' i! III it ¥ fa 2 1 B' ..... -...-..---... ~ • ....--. - ~ ........ .., .... .- - 01
34 U 30 21 26 24 2t 20" 16 l' 11 10 a 64 1,1 n 7 i I 13 i .-7. i 21 nT FJ: ~ -: --. · ' .. -.-...:..- -...- • ---e. ~~.Ji •• -'-. ~- --: - .-
_ II - f - 'l '1- ~ ~t ~, 'l _ ~ _ ~ _ 20 . -~ .
100
L. I
-- -
0 -N -..t
395
1430
I .-1. , !
-r+1 -
! j~ JUL f---i ib -- r-fi
,
18 b
375
l Beginning of door
End of convergent
r 50 ---,
.. i+. _ "i -- ~ K 0_ -\~il!& - - N
21 -to --;.,- . 50 J
•• I 180
-:!I5 3$ I
Section axis End of door
Diagram of wall pressure recorders
I%j ..... lQ c 1"1 ro '-J
Figure 8
Equipment of adaptable cryogenic walls: specs of pressure recorders, jacks, and thermocouples
Wall pressure recorders Jacks --
I }~PH XP8 ZP I ~~?H ):F'8 ZP I 1,)1' (",','
1 -812.5 -812.5 213.13 4'~ 2613.0 260.13 213. ~3 1 ·-i'05.1:J
2 -787.5 -737.5 -213.'3 59 2.,e.eI 2913.'3 -2(1.13 :2 '-575.0
3 -747.S -747.S 20. ~J 51 3313. a 33'3.'3 20. ~3 3 '-460. ~3
4 -722.5 -722.5 -213. ~3 52 :;::na. '3 ~::3~J. 0 -2'3.'3 4 ·-~:55. ~j
5 -692.5 -6n.5 2e.~ 53 417.5 417.5 -2~3. '3 5 -·275.13
tS -657.5 -667.5 -20.la 54 442.5 442.5 213.0 6 "215.0
7 -63a.~3 -638.13 -2'3.13 55 467.5 467.5 -2~3. '3 7 "155. e
:3 -592.5 -592.5 28.a 56 492.5 4'32.5 2a.~ :3 -95.9
9 -567.5 -567.5 -20. ~3 S7 517.5 517.5 -20.'3 9 -35.0
11:'1 -5313.13 -530.13 -28. () 5~ 542.5 542.5 213. ~3 10 25.13
11 -492.5 -492.5 28.0 53 -630.0 -63~3. '3 2~3. '3 11 85.13 12 -467.5 -467.5 -2e.() 60 -5313.8 -5313.13 20.'3 12. 145.13
13 -442.5 -442.5 28. ~I 61 3813.9 3S~.'3 28.13 13 2t1S.0
14 -417.5 -417.5 -28.0 62 -735.8 -735.0 -133.0 14 285.13
15 -:332.5 -392.5 28. ~} 63 -530.8 -5:313. a -133.1} 15 330.0 16 '-367.5 -367.5 -28.0 64 -33'3.13 -330.13 -133.~3 16 505.13 17 '-338.0 -338.'3 221.121 6S -288.13 -2130.13 -133.'3 P --2::13.13 -298.13 -29.121 66 -1~1:3.13 -1£lI3.a -13:3.~3
'J
1 " --2613. ~ -268.'3 213.0 67 -4'3. ~3 -413.13 -133.13 21) ·-23'3.0 -230.9 -213.0 68 a.a 13.0 -133.(} 21 '-2138.13 -208.13 213.13 69 4a.0 4~. ~3 -133. ~3 THERM. :22 --178. a -178.0 -2a.~ 713 lea.e 1013.'3 -133.13 ... ***io* "',' "145.13 -145.£1 2El ;·13 71 213a.13 20'3.£l -133.~ ,;,.J
24 -'128.0 -128. ~3 -213.0 ~ . ., 3313.0 ~:3e. e -133.'3 t ...
25 -·Hla.~3 -HI0.e 213.0 73 538.13 5313.0 -133.0 I ><TH "'- -85.a -85.13 -28.13 74 -735.13 -735.13 133.Q ..:.::. 27 -78.13 -713.0 28.'3 75 -€-38.'3 -639.8 133.13 8 -~~3? '3 23 -55.0 -55.13 -28.13 76 -5313.13 -530:9 12:3. I) 7 0.13 29 -413.13 -4e.a 28.a 77 -439.8 -4313.13 133. '3 9 475.13 39 -38.13 -38.0 -28.13 78 -3313.13 -33'3.13 133.13 31 -213.8 -213.8 28.0 79 -260.e -2613.0 133.0 I :r.:TS 32 -10.13 -18.13 -213.13 8a -2al3.a -21313.8 133.13 -:") 13.13 8.a 213.13 81 -145.13 -14-5.13 133.13 6 -7'37.0 -.. "J
34 la.a 19.8 -213.13 az -1813.8 -11313.0 133. ~J 4 -427. ~) ~:5 28.13 29.0 28.0 83 -713.13 -7~.~ 133.0 2 -1813.~J
~:~ 30.13 38.13 -28. ~3 84 -48.0 -413.13 . 133. a 1 ~.~
37 43.0 413.8 28. 13 8S -28.a -29.13 133.'3 3 17'? I) ~,~ 55.13 55.13 -Z8.e 86 '3. 13· a.e 1:33. ~3 5 479. ~J " .. "J
39 70.0 7'3.8 za. ~3 97 Z0.e 213. ~3 1:33.13 .. P3 78.8 78.3 -20.13 88 48.13 413.13 133. 13 41 91.3 91. 3 28.0 89 78.13 7e.e 133.0 42 laa0.0 100.\3 -213.'3 9'3 lee.a 10e.'3 133.1) ...... .,..,:, 123.13 12e.0 28.0 91 139.8 133. a 133.13 44 ll38.8 138.8 -2E1.13 92 200.13 20~3. 13 133.0 45 151.3 151. 3 28.8 93 260.13 269. ~3 133.13 46 ],70.13 178.13 -213.13 94 3313.\3 nO.a 133.13 47 &:013.13 28e.a 28.13 95 430.0 430.13 133.13 43 2.30.13 2313. a -zEI.a 96 538.13 539.13 133.13
XPH-.XPB-XV-XTH-XTB IN MM/AXIS PORTHOLE Z in mm/section axis
38
Figure 9
Pressure recorder sE§cifications - lateral walls (mm)
upstream hole central hole N I X Z II N X I Z
----1----- -----11---- -----1-----1 I +15Q II 2 1-375 +100 II 3 I + 50 II
----1----- -----1 4 1-455 I 5 1-410 1 6 1-375 0 I 7 1-335 1 8 1-295 1
----1----- -----1 9 1 - 50 I
10 1-375 -100 1 ~ 11 I -150 I ~ ____ I _____ ----_I
1 1+160 :2 0, 1+140 :~ 1+120
----- 1-----, 4 -120 1 5 - 80 1 6 - 40 I , 01+100 EI + 40 I 9 + 80 I
10 I + 12 0 1
----1-----1-----11 1 1+ eo 12 1 0 1+ 60 13 1 1+ 40 14 1 1+ 20
-.--- 1-----15 1-160 16 1-140 17 1-120 19 1-100 19 1- 80 20 '1- 60 21 1- 40 22 - 20 23 0 24 + 20 2S + 40 26 + 60 27 + 80 28 +100 29 +120 30 +140 31 +160
o
1 .1
1 -----1
32 33 34 35
36 37 313 39 40 41 42
o
-120 - 80
1- 40 I 0 1+ 40 1 + eo 1+120
--.. - 1-----4:~ 1 4'1 1 0 4c' •• 1 ___ ._ 1 ____ -
- 20 I -'40 J - 60 - eo
-100
-120 -140 -160
downstream hole 1 N X I Z J 1---- -----1-----1 1 1 1+150 1 I 2 +375 1+100 I I 3 1 + 50 I 1---- -----1-----1 1 4 +295 1 I 1 5 +335 1 1 1 6 +375 I 0 1 I 7 +415 I I 1 e +455 I I
1---- -----1-----1 I 9 1- 50 1 I 10 +375 1-100 1 1 11 1-150 1 1 ___ 1 1
39
Figure 10
Diagram of the win~
AS07
4
-E E ...,
N 3
4110
2 -20
1
0 ..
0 X (mm) 0 .. .. 40
Figure 11
Specifications of the AS 07 wing
A B.A. B.F.
I Y I X I ,< 1 corde I (rom)
------------1---------1---------1---------1---------1 B _::::~::~~~_ : ____ ~ ____ : ____ ~ ____ : _~~~.::::_: _:~~~:::_: c __ ~~::~~_~ __ : __ ~:~:~ __ : ___ ~~~~ __ :_:~:~~: __ :_~~~~~~ __ :
ra"qee 2 1 30,34 1 17,88 I 146,12 1 128,24 1
------------1---------1---------1---------1---------1 ra"qee 3 1 60,40 1 35,6 1 144,15 1 108,55 1
------------1---------1---------1---------1---------1 I:'tlpttlre 1 75) 227 i 44,335 1 143,18 1 98,845 1
------------1---------\---------1---------1---------1 ra"qee 4 1 104,301 1 61,47 1 153,61 1 92,14 I
~-----------I---------I---------I---------I---------I ra"qee 5 I 196,41 1 115,75 1 186,66 1 70,91 1
------------1---------1---------1---------1---------1 ra"qee 6 1 279,87 1 164,94 1 216,60 1 51,66 1
------------1---------1---------1---------1---------1 J) :iatlmo" 1 309,60 1 182,464 I 227,264 1 44,80 1
---------------------------------------------- ______ 1
Key
A - chord B - root C - row C - tip
41
• &0
FigurE~ 12
u , N
Key
Position of pressure recorders for each section
A ~~ __ ~~~~ ____ ~_~~~~~ __ ~ ___ ~_~ ______________________________ : B 1 Extrado~ 16 pri5e5 1 3 5 8 12 16 20 25 30 % 1
1 1 35 40 50 60 70 15 80 90 \ 1
I----------------------------~----------------------------I t 1 lntrado$ 9 prie.es 1 3 7 15 30 45 60 75 85 \ 1 1 ___ • __ -----------------------------------------------_______ 1
Profiles
-------------------== -..- -=::::
A - B.A. 1 recorder 16 recorders
8 recorders B - Outer section C - Inner section
42
Figure 13
~pecifications of pressure recorders on "Airbus" AS07 wing
10 25
'~.- -=+ • I
r-----------------------------------------------T~-----------~----------------------------------,
t--------.- --fl--T ~~ ~~ -~ -~::~ ~:~ -T ---------------1-------____ IJ. --T ~:~~- --~::~::~-T------------ --- ~ co I range,. 1 I rango. 2 I rango. 3 I reng... 4 I r • .iv..:1 I ranIJ.. 6 I
I V - 7.:l60~m I Y - 30.340m. I Y - 60.400~~ I Y -104.301 ••• I Y -196.410 .. I Y -279.870-. I I---------------~---------------~---------------~---------------~---------------,---------------l
J) IB.A.- '1.295,"" IB.A.· 17.715 .... IB.A.· 35.498", .. IB.A.- 61.392." .. IB.A.-115.701 .... I.B.A.-114.143_ I f IB.F.-147.620m .. IB.F.-l'16.120"". IB.F.-14'1.150m .. IB.F.-153.610.nm IB.F.-186.66o.". IB.F.-211.600.". I ~lcordoI43.160m .. IcordoI29.2'10", .. Icordol0B.550 .... Icord" 92.1'10'010 Icordo 70.910 .... Icord. 51.6600". I
I X hom) I Z (mm) I X (m .. ) I Z (mm) I X (mm) I Z (10m) I X (mm) I Z It.m) I X (mm) I Z ( .... ) I )( It.",) I Z (.".) I
r .. -~-------~-------,-------,-------,-------,-------,-------,-------,-------,-------,-------,-------l 11125.9791 -1.0601126.7531 -.9121127.7'1'11 -.4771139.7961 -.4271176.01'11 -.5291209.8021 -.6111 21111.6521 -2.0301113.9'161 -1.6031116.B601 -1.1041130.5461 -1.0591169.8831 -1.0621203.6551 -.9401 31 90.2251 -3.3931 94.6431 -3.0431100.6961 -2.3491116.6091 -2.0471159.1921 -2.0951195.9771 -1.6861 41 69.7031 -4~1001 75.4761 -4.0261 84.4441 -3.4161102.910) -2.9411147.6761 -2.9361188.1101 -2.24'11 51 47.0661 -2.6701 56.0691 -3.4111 69.0841 -3.1551 99.0961 -2.6831137.0291 -2.7391180.3791 -2.2341 61 25.7418 .8331 36.7851 -1.1561 51.7531 -1.6801 75.2791 -1.4041126.'1441 -1.9331172.7751 -1.6851 71 14.6241 3.7941 26.5601 .9241 43.0911 -.1991 67.9091 -.3441120.6611 -1.1601169.5321 -1.1591 91 8.7511 5.7831 21.2491 2.3951 39.9731 .8691 64.1741 .4591117.7681 -.5311166.4871 -.7421 91 4.2951 10.8001 17.7151 6.3271 35.4981 3.9231 61.3921 2.9091115.7011 1.3021164.9431 .6311
101 8.7231 15.4931 21.7701 9.9861 39.9401 7.0701 64.2671 5.4671117.9731 3.3231166.5471 2.0251 111 11.5951 16.1991 24.3581 10.4871.41.1051 7.4961 66.1081 5.9431119.4171 3.5991167.6341 2.2031 121 15.9461 16.6471 29.1291 10.9231 44.2831 7.9491 69.8971 6.1101121.5011 3.8351169.0651 2.4421 13121.6181 16.6041 33.2521 11.2531 4b.6401 8.1841 72.6441 6.4091124.4221 4.0571171.2781 2.6761 141 27.2771 16.4891 39.4121 11.5291 52.9g11 9.3151 76.3131 6.5991127.2901 4.2571173.3751 2.8091 151 32.9111 16.2591 43.5671 11.6341 57.3g31 8.4901 80~0391 6.7451129.9931 4.3201175.4301 2.9221 161 40.3451 15.8321 50.1301 11.6211 62.7711 9.5391 84.7001 6.7841133.4731 4.4401177.9311 2.9541
1171 47.3781. 15.3251 56.4151 11.5521 68.2031 8.5991 89.2201 6.73111137.1561 4.4991190.6421 2.9741 1181 54.6001 14.7791 62.3671 11.3731 73.6291 8.5591 93.7971 6.6741140.6191 4.4421183.0361 3.0241 1191 61.8171 14.1091 69.2751 11.1231 79.0511 8.3301 99.3531 6.5571144.2141 4.4391195.8511 2.9851 1201 76.0801 12.5931 81.9701 10.4771 99.9051 7.9861107.6211 6.1191151.2501 4.1161190.9361 2.8621 1211 90.3931 10.9711 94.8431 9.2691100.7071 7.1621116.9091 5.5641158.2431 3.8241196.0001 2.6491 1221104.7291 8.9911107.7031 7.9231111.6691 6.0901126.1681 4.9141165.5011 3.3311201.1001 2.3121 1231111.8391 7.8691114.0701 6.9611117.0011 5.5601130.6411 4.3111169.9271 3.0091203.9411 2.0561 1241119.0201 6.7011120.4921 5.9801122.4671 4.9461135.2041 3.7471172.3671 2.6291206.3491 1.9501 1251133.2691 3.9201133.~)11 3.6261133.3041 3.0711144.3551 2.4271179.5521 1.6941211.6141 1.1811 L __ l _______ ! _______ , _______ £ _______ ! _____ •. _~ _______ l _______ ~ _______ ! _______ ~ _______ ~ _______ J _______ J
A Internal wing B External wing C Row D B.A. E B.F. F Chord
43
CONTROL TESTS
Wall incidence and rotation:
Convergence of iterations:
Non/2-D/3~D comparison:
Figures 14 to 16
Figures 17 to 20
Figures 21 to 23
44
A - Non-adapted B - Wall shapes C - Row D - Upper wall E - Lower wall
Key to fi~res 14, 15, and 16
F - Central rows of pressure recorders
45
,
I. M=O.6 .
"0120 I a. =+20 A0122
,._, J
• ~ ~ 1:
A non ada pte
0_ AD120 ::0 0
• te::....- I : • __ AD122 . rt OJ rt
18-::J .. I"%j 1-'-
-I' I
l .. ~~--~_t"1
.70T I , I· • I . m
rt
U I c: Rangee@ ()
«
I I~ •• 11. 1: Parol haute D
I-'
•• 0. s.-. ........... ...-n .... ~ x/c • ••
Paroi basse E I ~ ~ ~ I
- . .lIsl
Rangees centrales de prises de pression F
X (mm) I"%j
• 1101 I I I 1-' •
v 0 9 0 lO .C) 0 0 c 0 II 1\ t"1 .. I I CD
~
0"1 I-' ~
•• 0
.. " •• 0
• 7.
.70 0 0 0 ..
~
-....J
I.
•
o
-.. I
A0108
A0139
.B Formes des parois
a.e
~- .. .... ....
I.e
"
, , , , , .... .... ............
M=OI8
0.=00
A non adapte
0_ AD108 + __ AD139
Rangee@
C.
:u o rt' \11 rt' 1-'. o ;:!
I··
til (!)
o o :::s 0..
I , " XP U 0 I « 0 f: :!: I .•
... 1 Il I I
" X/C
£ Parol basse
F Rangees centrales de prises de pression
X (mm)
0 0 0 0 0 II II I
~ ~ ~ ..
~ 1-'. lQ C ~ It>
I-' VI
" '" ;
01:>0 CO
'0 Tn.. "N /'
. ~-• .c......
-.. ... ~ '·°1
•• 0
o Paroi haute
~ ........ L ._ ~ -;~~.~
• £ Paroi basse
~AD119 AD141
B Formes des parois
o 1
••• Itt
II \,,_
.. .11 ~----
..
\ M=O,8 \
L?-::~c , A adapte 3_D
0_ ADl19
+ __ AD141
c.. Rangee@
1-3 !:J" ..... 1'1 0..
(") o
...I I~/c ~ ~ ~ r •
.'7. F Rangees centrales de prises de pression
X (mm)
• '701 0 o 0
g f .. •
0 0 0 a
I ..
~ ..... lQ C 1'1 CD
~ 0\
_.
First case
•• Il. A , N Form" des parolS
•
o
•• 0
• · • I
.J X
\ C. • If!\ ' Rangn \¥I
-L ".. \
XP
: •
0_ AD 105 (0) • ___ AD 115 (1)
• _, AD '16 (2)
_ •••• AD9116 (3)
\::::: ==.::::=:-:.:::::::::::::::;:;~:::=== ------- --O::::::::::==~~
..
....... ----~ I ~ •
!5~
A - Wall shapes B - 3-D convergence, no rotation C - RO\lI
x/c
Figure 17
49
.e Il N
e
e
.. •.• J-_____ _
~ .
Kex.
A ... Wall shapes B ... Row
o o • I
Second case
•
XP
: • o : CI_ AD 126 (0) • ___ AD 127 (1)
._. AD 128 (2) .• __ AD 129 (3)
• ____ AD9129 (4)
X/C . ~
FigurE? 18
50
A - Wall shapes
1.1
I.'
.'
..
•
c. ~ Range.®
'\.
o o 1
• o . •
Sans rotation
XP
: •
\ \. ~~-~. ~-;;:~~.-~.~~
~;,--- ~-....::: .. ........-;;:: ~
. . ---=::----==--.D
AD133 (depart A04) • _ iteration (0)
(1)
(2) .. (3)
x/c .,.~----"""',----------"!--_--"'"
I ~ ~ ~ ~ .; -
B - 2-D convergence, no rotation C - Row D - Beginning
Figure 19
51
1.1
..
1.1
: •
Key
I.
•
•
-10
A Q. Forme-s dH porois N
~
o o . I
A - Wall shapes B - 2-D convergence, no rotation C - Row D - Beginning
~
o
! M=o,a! --~ a=Qo
.B Conv~rg~ncl! 2-D
Sons rototion
XP
g . g •
j) A0134 (depart AD133)
0_ iteration (1) (2)
._. (3)
.__ .. (4) x/c
, ~ ~
Figure 20
52
A - Wall shapes B - Row C - Upper wall D - Lower wall
Key to figures 21 and 22
E - Central rows of pressure recorders
53
Figure 21
Non/2-D/3-D comparison
..,...,. ........ _---.... ,.:....-_ --·---AO\35 2-0
,,.,-:;"/ _. __ ~ ... ADI05 non "l:!t .. .".--~............. .~ . .~ - , "'AOll6 3_0 '.0
. A FormH d~s porois
.Ia.
.[.~T~ .. --....~,.
~ ... -I. f !
,
:r u «
, .va :r
• vo
.11.
XP -
..
•••
..
..---~~~~---- =--::.B Rong.~ <Z>
----_ . B Rang •• C5> ............. ---=:::::::::::
__ AD105 non ada pte
• __ AD135 ada pte 2_D __ . ADl16 odopte 3_D E Rang."s centrales d" pris". d" prllssion
X (mm)
eliOt'"" -- '--;:-----.... , ----.:.. ..
. ~ O! O.O;-____ -m ___ ~~-------~H~/:C
: m ~ ~ : ..
54
...
I I
Figure 22
Non/2-D/3-D comparison
. c., A FormH des parols
~~ ....... ...
~ -.. . .......... , , ! - XP • i
I , Rongt.s c"'lro~s de prlsn de pression
X (10m) I • -<
I
..
~:---:Jlr----;r' - ___ --- )(/C
~ ~
'.0
..
111.0 o o .;
)(/C -.:
55
o
-,
/2 -D/3-D corn Non parison
non . LD tat ion . __ _
Adap . 3_D
-~ O· "CSence: 1nc.
. .: 0,8
3
:> X (mm)
!
• •
:
Figure 23
®
.@
®
56
VISUALIZATION OF CURRENT LINES
ON THE LEFT LATERAL WALL
Mo = 0.6 oL. = +2· Non-adapted Figure 24 Mo _. 0.6 cl.. = +2· 2-D Figure 25 Mo - 0.6 01-= _2· Non-adapted Figure 26
57
Figure 24
Left lateral door visualization ~= +2· M = 0.6 non-adapted
58
Figure 25
[illegible]
59
Figure 26
Left lateral door visualization ~= -2· M = 0.6 non-adapted
.. --- :=:3 - -~ .. - -.
--=;. -
60
Use of four base cases
o
H-O ,6 0,8 .----------.
147 (*) 122 (**) 1 167 (***) 1
----------1----------. 150 (*) 1 153 <*) 1 107 c**) 1 lQ3 (**) 1 162 (***) 1 165 ( ;,**) 1
----------I----------! 136 ( .... ) 1
159 (***) 1
----------!
H-O,6 0,8
1 1'46 (*) 1 +2 1 1~5 (**) 1
1 B~ (**"'ll
I----------I---~------. 1 14:: C*) 1 152 (*) 1
a 1 136 ( ... *) 1 134 ("'*) 1 1 162. <***ll 164 (***) 1 I----------I----------! 1 155 <*) 1
- '2 1 144 < ** ) 1 1 158 (***) 1
!----------! H-O,6
1 148 (*) 1 "'2 1 123 (**) 1
1 1S:3 < ***) 1
0,9
1----------1----------. 1 1S1 (*) 1 lS4 (*) 1
o 1 11 7 ( ** ) 1 119 (**) 1 1 163 (***) 1 lSS (***) 1
I----------I----------! 1 157 <*) 1
-2 1 143 <**l 1 1 lSI) (***) 1
!----------!
Shape of walls Mach on adaptable walls Mach on lateral wall Kp distribution Lift coefficient
NON ACAP,.E
<*) ranqees 1-4 <**l rang~e$ 2-5 (***) ranqss3 3-6
AD~P"E 2-D
ADA?1'E 3-D
Figures 27-28 Figures 29-32 Figures 33-36 Figures 37-44 Figures 45-50
Figure 26a
61
Use of the four base cases - Wall shape
,0
-::
o
-.0
o o . I
o : I
a. N
a. N
; I
: . I
~~:::::=::;;:~:- 1.0144 adapW 2_0 ~ 1.0142 non ada pte
1.0143 adopW 3_0
-""'-It.::;;;::;:::;:::::,;;;::.:=-_ sans rotation
XP
i AD 122 non adapte
• rotation 30'
- • rotation 30'
------------ so.ns rotation
o o :
XP
o o •
"Sans rotation" = No rotation
Figure 27
62
Use of the four base cases - Wall shape
I.
•
• : . I.
•
•
I I
n. N
n. N
I MoO.S! a.= o·
o ~ •
! Moo.a! a.= O·
! I
"Sans rotation" = No rotation
-..........
•
•
--""
adapte 2_D non adapt.
-...... sans rotation -..... XP
• t • o .
: •
Figure 28
63
Key to Figures 29, 30, 31, and 32:
A - Left lateral row B - Central row C - Right lateral row
64
Figure 29
Use of the four base cases - Mach of adaptable walls
.70
... -"
A0142 non odopte .BB
x (mm) .. 0.1------_, ___________ _ g o i ...
•• 0
....
I U ~ 1:
o
A •. ... rangre klt«alI! gauc:hl1 ~ . _ rangre c~rQIe '- ••• rangH Iat~ droit.
_ ... __ ............ : .. : ..• ,~ •• --4~~
A0144 odopte 2-D
x (mm) •• O'~ ________ ~, _________ ~ ____ • _____ __
... .80
o o ~ •
.BB
o o ~
t' •.... ·a ....... ~ .......... ~
x (mm) .H,~-----___ -.· __________ ~----------~
g o .. •
o g •
65
Figure 30
Use of the four base cases - Mach of adaptable walls
•• 0 ~ - .... . .. -,,'ft······ ... ~~ ... ~. -'" .
A0107 non odapte ... x (mm)
.~--------~.----------~----------~ .110
0 0
~ •
•• 11
I U ~
•• 0 l:
.1111
.11
0 0
~ • ....
I U ~
.110 l:
."
.110
0 0
~ I
o , o
A ... " fClngH IateraJe gauche B ' - rangH cmrall? c... .- - rangH laterote droit.,
• » .. ~
----...... "icd! .. ~~~ Iait
CI CI .. •
-
g II I
o
o
A0136 odopte LO
x (mm)
o o ..
AD117 odopte 3_0
x (mm)
66
Figure 31
Use of the four base cases - Mach of adaptable walls
.70 I: U I M=o,61 < ... l: a=+2°
•• 0 >. o~ .. 'O
• ell AD122 non adapte
X (mm) .eo ---1
0 0 0 .. 0 0 0 ~ , IS I
A 0000 0 rQ~ Iat«CIIe gClUClw . .., 5 0_ rQngH c:.ntrQ( • I: C ._- rQngH tat.rcu. droit. U « ~. .... l: "'.~ ,... = ....... ~.......=;4:::c.~
--~- - ...
A0145 adapte 2_0 .eo
X (mm) ---1
0 0 .. 0 0 0 0 ~ • IS I
I
... I: U « ~ l: >- .... ..., .... '
•• 0 ...... ~ ... -: . ,', .. . ' ....
A0123 adapte 3_0 .... X (mm) .... -
0 g .. 0 0 0 0 , • .. I
67
Figure 32
Use of the four base cases - Mach of adaptable walls
." r u < ... l:
•• 0
AD108 non ada pte .'111
X (mm)
.'10
0 0 0 0 0 0 0
~ II II
• • • •..• ~~~g~
.. 8. . _ rangft c.ntralf
r • __ rangH ~alf droit~
U < ~ ......
•• 0 l:
" .. -'
A0134 adapte 2-0 .'111
X (mm) .'10
0 0 0 0 0 0 0 ~ II II
• • ... r u c(
.110 l:
A0119 adapte 3_0 .'1.
X (mm) .'1
0 i II II II 0 : I • I
670..
Key to Figures 33, 34, 35, and 36:
A - Vertical rows D upstream
middle downstream
B - Horizontal rows o upper
middle lower
68
Figure 33
Use of the four base cases - Mach of lateral walls
.70 I Or? u ...... <{ E 1: .§ ...
>-
" . _TfjQ5 MAC~ · . . · . · . · . · . • eo ~-- AD142 non adapte
.70 1: I U'E <{ E
•• 0 1: ....... >-
X (mm)
o
I~-TMAC~ . . . . .. . 15
RangHs yfliica(H
• Qmont m~iQ~
• aval
•• 0 ------.----- AD144 adapte LD
X (mm) .M.~------_________ ~
o ~ I
'70I~ I~ <I: E .•• 1: !
>-
o o o •
MACH Tfi
~~ horizonta(ps
• SUPffNH __ rMa.anps
inf'rleurH
.eo ~-- AD143 adclpte 3_D
X (mm) --, o I
69
Figure 34
Use of the four base cases - Mach of lateral walls
0rlS ~j~~ __ ~ __ ~_M __ A.CH .10 :r •
u ..... • « E • ~ E •
M=O,6 a=oO ... ~ ...... .
.~
~ ....... ~--•• 0
x (mm)
"
.10 I rTl-: U E . « E :
.ID l: >-
I I •• 0 ------~.~.~~~------""
x (mm) .... 0 0 " II I
AD101 non ada pte
MACH A
B9.!lg~ ...rtic:al.,
• omant ~ian"
• avaI
AD 136 adapte LD 1> 8,gngHs horizontal.,
• superMoutH _ median"
• inf.rieul'H
MACH
'7°1~ I~ ... 1:
~
~--'--I "!----I'
.... ~ AD117 ada pte 3_D
X (mm)
.HO~----------~ .. -----------~I , I
70
Figure 35
Use of the four base cases - Mach of lateral walls
.?o:rOr' l~ u ..... • < E • 1: E • . .a;: .: r 7
MACH
.80 ~2~ AD122 non adapte
x (mm) • 50 oJ-__ ---:-.-----I~
f :
____ ---,_-,-....:...M:..:..;,A C H
]rIG I; >- •
x (mm)
.lIe.l------- t o .. 0 o 0 o • I
,..._---,_~-M:...:.:A. CH
·"~~r 1/ .... :r >-
A 8£ng.es vertical.s
• amant m~ianH
• oval
RangHs horizantal!!s
• sup.r ieures _ m~ianH
• inf.rieures
•• 0 ______ ~ AD123 adapte 3_D
x (mm)
.DD~-----_·----_I gog ,. .
71
Figure 36
Use of the four base cases - Mach of lateral walls
AD108 non ado pte
x (mm)
.711 - -.. .. .. .. .. • • I
MACH Rangm ".,-tical.,
.... 5~1 I • amant rMdianH
< E . oval 1:
..... .
." >-
.... ~~~. A0134 adapte 2_0 8.9.!lgm horIzontat.s
X (mm) . sup~i.ures _ m~iQn.,
.711 --.. I .. .. .. inferi.ures .. .. . • • I
·MACH .... ~~1 f . -1: .....
>-
.... --------~ A0119 adapte 3_0
X (mm) . .,. - I .. .. .. I .. I •
72
o
o
.,
Use of the four base cases - Kp
•
:0,6
• o
....... -
•
non
•
t\.. •.•.•••• _ '.
o '. '. '.
• •
AOt42
"'" )( . .. ~~. -F--':::"':':':-':':'" ~"'_' ---...... AOt56
'. o
...... )( c .......
o : AOt59 c..... ____
......................
"" "'1.--....... )IE c .........
• ~ ..... -••. ,....; .. ~ .• ;;:.--== ...... -.::____ AOt42
................ ~ "..... )(
--.-.... --.--.. ;:.. .. -=:~----"""""'--j""'---
AOt56
)( I
-~ X (mm)
Figure 37
®
®
73
_&
Use of the four base cases - Kp
&
non ~daptet1on 2_0
3_0
~ 2· incidence: -co
~ech : 0,6
o
o
•
H--------~ S;;;;; ==:-:
x (mm)
)(
!
)( I
:
. ..
:
Figure 38
®
®
®
74
.,
Use of the four base cases - Kp
p.dl!lptetion non
,.-inCidence: O·
HOC" : 0,6
o
o
• +-----..:...-.:,~)( @) I
_____ .--:----. AD 107 ......... ... ........ - ~
.•.• .....)IE @ ............ \::::::!.J .. ..
"'-'-"'" ~0150 ............ ,,'" .................... ..
............ _-.. @
_ .•.... ----------... _------........•........ -----.... -.......
A0107
)( ® • :
A0150 .. --------------_ .. --_ ............. _ ... j.:----: • • ..
-~ X (mm)
)( I
Figure 39
75
.&
Use of the four base cases - Kp
non
Ad e ptet10n 2_0
: 0,6
o
o •
3_0
o
•
o :
)(
• :
)(
• ~
)(1
!
x (mm)
:
)0(
.. ..
)0(
• •
Figure 40
®
®
®
76
Use of the four base cases - Kp
A
Ad8ptet ion 0 non
tneioenee: .2· Maen : 0,6
)IE
a a
)IE '. --....
/0""
------~ , ..... -......... ----........................ ... +--..,. ....... 4 ........ _ .. __ _
-===------..................... . ... -....... .:. ........ '*""--:-'~-- .... _--
.. ...
• • A0167
)IE
A0122
)IE
! ------ AO~47
............. _-----_ .. - ............................. _- ---*-----~--~~-~-,-
" " ,-
-~ X (mm)
)( I
:I ..
Figure 41
®
®
®
77
o
f the four Use 0
tet10n ,A.dep
s - Kp base case
........ _- ..
• :
)(
• :
"'.$ .... ~~ I
I 0 .. : ;>
X (mm)
Figure 42
®
.®
@ • •
@
®
CD
78
..
Use of the four base cases - Kp
,Adl!lptet ion .non
incidence: Q. +-.--....:...:--*)I(@
0,8
......... -._--........ '. ' .
:
---.~.,. ••••• AD108
'. "
.................... , -..
.........
'"
. ..
AD153
)I(
• e
AD165
)(
• : .. ----- .... ~
-..• .••••••••• ••••••••• • •••• ~ •• ~......... c. ADIOS
)(
• :
.... -.--~ .......... . .....•...... ~ ....... ~ AD153
: . -~ X (mm)
)( I
!
®
®
Figure 43
79
.l
f the four Use 0
Adept2lt1on
o· incidence:
: 0,8
:
__ non __ ._ LD
_ .. LD
s - Kp base case
-~ X (mm)
)IE
)(1
: ..
:
Figure 44
®
@)
®
80
Figure 45
Use of the four base cases - Cz Cz recapitulative
Local lift coefficients
r-----------~----------------,----------------T----------------~ I I NON ADA PTE I AOA?TE 2-D I ADAPTE 3-D I
~-----------+----------------+-----------.-----+----------------~ I I R 1 0.3600 I R 1 0.3405 I R 1 0.3027 ! I I R 2 0 . 3726 f R 2 0 . 3687 I R 2 0 . 3229 I I I w +2 f R 3 0 .4388 I R 3 0 .423:7 I R 3 0 .3:752 I
H - 0.6 R 4 0.4740 R 4 0.4715 R 4 0.3861 R 5 0.5091 R 5 0.4948 R 5 0.4127
I R 6 0.4348 I R 6 0.4250 I R 6 0.3658 I
~----------------+----------------+----------------~ I I Aile.: 0.448 I Aile: 0.438 I Aile: 0.371 I
~-----------+----------------+----------------+----------------~ I I R 1 0.2081 I R 1 0.1995 I R 1 0.1865 I I I R2 0.2154 I R2 0.2198 I R2 0.1984 I I I ".' 0' I R 3 0 .2711 I R 3 a .2537 I R 3 0 .2411 I I H" 0.6 I R 4 0 .2418 I R 4 0 .2419 I R 4 0 .2076 I
IRS 0.2351 IRS 0.2337 IRS 0.1984 I I R 6 a . 1993 I R 6 0 . 1926 I R 6 0 . 1647 I
~----------------+----------------+----------------~ I, I Aile: 0.231 I Aile: 0.227 I Aile: 0.200 I
~-----------+----------------+----------------+----------------~ fiR 1 0.0798 I R 1 0.0661 I R 1 0.0687 I I I R 2 0 • 0881~ I R 2 0 . 0819 I R 2 0 . 0799 I I - -2 I R 3 0 .0989 I R 3 0 . 0949 I R 3 0 . 0945 I H· 0.6 I R 4 0 . 066!5 I R 4 0 . 0632 I R 4 a . 06 07 I I R 5 0.0561 IRS 0.0440 R 5 0.0486 I I R 6 0.0232 I R 6 0.020:7 I R 6 0.0174 I I ~-------------.---+------------..... ---+----------------_l I I Aile: 0.06E; I Aile: ~.059 I Aile: 0.052 I
~-----------+----------------+----------------+-----------------1 I I R 1 0.2401) I R 1 0.2253 I R 1 0.2034 I I I R 2 .0 . 2 5 4~5 I R 2 0 . 2509 I. R 2 0 . 2128 I I I - 0 I R 3 '0.3082 I R 3 0.2842 I R 3 0.2488 I I H - O. 8 I R 4 0 . 375 ei I R 4 0 . 3341 I R 4 a . 3 026 I I IRS 0 .415 () I R 5 0 .3825 IRS 0 .2853 I I I R 6 0.4162 I R 6 0.3193 I R 6 0.2555 I
I ~----------------+----------------+----------------~ I I Aile: 0.353 I Aile: 0.315 I Aile: 0.263 I L ___________ ~ ________________ ~ ________________ ~ ________________ J
"Aile" = wing
81
Figure 46
Use of the four base cases - Cz
.~ 0 c - I I Q. N C") ....... 0
" -CII -c. E 0 - -0. 0. U c: 0 .g '" 0 -g > c: 0
0 + x
",,,,:;,,- / /j 0 ("I)
/
I I .
7 I r I 0 I I I 0 N I 0 I
I N + I 0 I
I I I
II I I II I
I II
I I tj tj I tj I
f
I I I
I I , 0 ,
t \ • N
I ,
I ., I '.
II I \ I I ., , ~! I
\ I I
I~ I
U) ,
\ \
I .. \ ~ C:> \
II ~ l :;( 0 . -:E \ ~. - ~ a" a ~ \\ c
u ~
0 $ - '\ .S
N· \<!..~ U \ . I .-< .. 0
LO ~ ("I) N - 0 ... ~ ~ ~ ~
0 0 0 0 0
Key
A •• Internal wing B .. External wing
82
0,5
0,4
0,3
0,2
0,1 A
Aile interne 0
()
A - Internal wing B - External wing
Figure 47
Use of the four base cases - Cz
M
0,6 0,8 «=0· 0 • non adapte
A , adapte 2_D
0 • adapte 3_D
• •
B
I I Aile externe Y(cm) .. 10 20 30
83
5
4
3
2
1
Use of the four base cases - Cz
Czxcorde (em)
-~ ...... ...JilL' .-... ... -:~.,. ":'- ....
.............. , .... . .......... --.'M-., ............ """ii ....
. -.. .. -\ ................
..-. . --.--
---" --. --'-"
FigurE~ 48
o non adapte + adapte 2_D )C adapte 3_D
'--.-.........:. a. 2°..-... A 11>-....;· - =-
Aile interne Aile ext~ie·-·-.~._. o o
A - Internal wing B - External wing C .. Cz x chord
,_ I
10 20
Y(cm) •
30
84
Figure 49
Use of the four base cases - Cz
M
0,6 0,8 a.= O·
0 • non adapte
A , adapte 2_D
Czxcorde 0 • ada pte 3_D
5 (cnn)
4
3 ~~ .. -~-- ----.. ----~
-- --~ III '-. ._......... • .... ---'-0-._'" --. ....-
'''~'' . .... ..... ---......... ..... ........ " .-............., '''0- .......... '-- -...... '--' ......... ~ '-- ........ '--.-- -.... - .......... 0- -"", ................ . ---.-.... ""'-"", -. ,
' ........ ""'- .......... ' ''''''''''0---'~
2
1 A .B' I '--~
~_A_il_e_~,_)t_e_rn_e~ _____________ A_ile __ e_x_te_r.n._e ____________ ,,_I ___ ~rn) o o
A - Internal wing B - External wing C '" Cz x chord
10 20 30
85
Figure 50
Use of the four base cases - Cz
A C A. 0,6 Cz aile 0,6 Zalle
.I o non adapt~ o non ada pte
0,5 + adapt; LD 0,5 + adapt~ 2.0 / • adapl~ 3_D • adapt; 3_D /
M=O,6 / 0,4 0,4 l
'I 0,3 0,3 1/
0,2 0,2 M .. 0,6 (T.N.) 0_
0,1 11 0,1 . -' M = 0,47 (T.D. 7·'.) ~. B compagn. Mars Yi117
f (:r.0 ao ° .. I I ~ ° '.., _4 _2 ° 2 4 _4 _2 ° 2 4
A •. wing B - March 1977 series
86
Fichier .- File Rangee .- Row Corde .- Chord
Listing of Cz
Annex 1
87
*****FICHIER * RANGEE : 2 * RANGEE : 5 **********
*****FICHIER * RANGEE : 2 * RANGEE : 5 **********
*****FICHIER * RANGEE : 2 * RANGEE : 5 **********
*****FICHIER * RANGEE : 2 * RANGEE : 5 **********
*****FICHIER * RANGEE : 2 * RANGEE : 5 **********
*****FICHIER * RANGEE : 2 * RANGEE : 5 **********
*****FICHIER * RAN GEE : 2 * RAN GEE : 5 **********
*****FICHIER * RAN GEE : 2 * RANGEE : 5
*****FICHIER * RANGEE : 2 * RANGEE : 5 ****** •• **
*****FICHIER * RANGEE : 2 * RANGEE : 5 **********
*****FICHIER * RANGEE : 2 * RANGEE : 5 **********
- 1 -
AD105 **** MACH = .702 INCIDENCE = 0.00 NON C2= 2.310E-01 CORDE*C:= 2.963E+Ol C2= 2.790E-01 CORDE*CZ= 1.978E+Ol
AD107 **** MACH = .599 INCIDENCE = 0.00 NON C2= 2.154E-01 CORDE*C:= 2.763E+01 CZ= 2.351E-Ol CORDE*C:= 1.667E+01
AD108 **** MACH = .801 INCIDENCE = 0.00 NON CZ= 2.545E-01 CORDE*C:= 3.264E+Ol CZ= 4.150E-01 CORDEle:= 2.942E+01
ADlle **** MACH C:= 6.918E-02 C2= 3.999E-02
= .697 INCIDENCE =~2.00 CORDE*C:= 9.872E+00 CORDE*C:= 2.835E+00
NON
ADl15 **** MACH = .702 INCIDENCE = 0.00 3D(I) CZ= 2.06~E-Ol CORDE*CZ= 2.645E+01 CZ= 2.215E-01 CORDE*CZ= 1.570E+01
AD116 **** MACH = .701 INCIDENCE = 0.00 3D(2) CZ= 2.050E-01 CORDE*CZ= 2.629E+Ol CZ= 2.270E-01 CORDE*CZ= 1.610E+Ol
AD11? **** MACH CZ= 1.984E-01 CZ= 1.961E-Ol
= .598 INCIDENCE = 0.00 CORDE*C:= 2.545E+01 CORDE*C:= 1.390E+01
3D(1)
AD11S **** MACH = .806 INCIDENCE = 0.00 3D(1) CZ= 2.070E-01 CORDE*C:= 2.655E+01 C2= 2.732E-01 CORDE*C:= 1.937E+01
ADl19 **** MACH CZ= 2.128E-01 CZ= 2.853E-01
= .805 INCIDENCE = 0.00 CORDE*C:= 2.729E+Ol CORDE*C:= 2.023E+01
3D(2)
AD120 **** MACH = .599 INCIDENCE = 2.00 NON C2= 3.802E-Ol CORDE*CZ= 4.876E+01 C2= 5.198E-Ol CORDE*CZ= 3.685E+Ol
AD122 **** MACH = .600 INCIDENCE = 2.00 NON C:= 3.726E-01 CORDE*C:= 4.~79E+01 CZ= 5.091E-Ol CORDE*C:= 3.609E+01
88
- 2 -
*'****FICHIER -: AD123 **** MACH = .61)6 H1CIDEHCE = 2.01J 3Dq) *' RAN GEE : 2 C2= 3.229E-~1 CORDE*CZ= 4.141E+01 * RANGEE : 5 C2= 4. 127E-01 CORDE*CZ= 2.926E+~1 ****':0:***** **HHl-F I CH I ER * RAt·IGEE : 2 * RAt-lGEE : 5 **********
***'H!FICHIER * ~:A~·IGEE : 2 '* RANGEE : S ****'*"if****
****-~FICHIER *' F:ANGEE : 2 *' RAHGEE :5 **********
*'****FICHIER *' RAN GEE : 2 * RAt-lGEE : 6
*****I=ICHIER * F:At·jGEE : 2 *' F:Ftt'IGEE : 5 *****,~****
***H·FICHIER .: *' RFtt·1GEE : 2 * RAt·jGEE : S
***,**FICHIER * F:AtK;EE : ~ *' RAt·IGEE : 5 **********
. *****FICHIER * RFtt'l(:;EE I 2 '* F~At·l(:;EE : ~ **********
*****FICHIER * F:At-lGEE : 2 '* RAt·1GEE : S **********
**~**FICHIER * RFtt'IGEE : 2 * F:Ftt'IGEE : 5 ****** .. ~***
AD124 **** MACH = .703 INCIDENCE· 2.00 NON C2= 4.071E-01 CORDE*CZ= 5.221E+01 C2= 6. 103E-01 CORDE*C2= 4.327E+01
AD125 **** MACH = .7133 INCIDENCE = 2. a~ 3D<t). C2= 3.361E-Bl CORDE*CZ= 4.310E+01 C2= 4.750E-01 CORDE*CZ= 3.368E+Ol
AD126 **** MACH = .806 It-lCIDENCE = 2.00 NON C2= 5.214E-01 CORDE*CZ= 6.687E+01 C2= 7.394E-Ol CORDE*CZ= 5.242E+Ol
AD127 **H' ~lACH = .806 HICIDENCE = 2.01) 3D(l) C2= 3.792E-01 CORDE*CZ= 4.863E+Ol CZ= 7.10SE-01 CORDE*CZ= 5.B36E+Ol
AD 123 ***'* t'lACH C2= 4.116E-131 C2= 7.5;21E-~1l
= .806 INCIDENCE = 2.00 CORDE*CZ= 5.278E+Ol CORDE*CZ= 5.333E+01
3D (2)
AD 129 **** ~lACH CZ= :3. '~n'E-IJ1 C2= 7. 4:=:5E-~11
=- . :306 I NC I !lEtKE = ;2.013 3D (:3) CORDE*CZ= 5.101E+Ol ~ORDE*C2= S.272E+01
AD130 **** MACH = .707 INCIDENCE = 1.50 2D CZ= 3.491E-01 CORDE*CZ= 4.477E+01 C2= 4.99SE~01 CORDE*CZ= 3~542E+al
AD131 **** MACH C2= 3.2!OE-01 CZ= 4.166E-01
AD 1 :34 **** t'1ACH C2= 2.509E-01 CZ= :3.8,:5\:-81
= .602 INCIDENCE = CORDE*CZ= 4.117E+01 CORDE*CZ= 2.954E+01
= .809 INCIDENCE = 0.00 CORDE*CZ= 3.217E+01 CORDE*CZ= 2.712E+Ol
2D
AD135 **** MACH = .702 INCIDENCE ~ a.0a 2D CZ= 2.384E-Ol CORDE*CZ= 3.05SE+01 CZ= 2.7S8E-01 CORDE*CZ= 1.9S6E+01
89
*****FICHIER ~ RAN GEE : 2 * RANGEE : 5 111*******
_***IFICHIER ; RAN GEE : 2 I RANGEE : 5 111*******
I*I**FICHIER • RAN GEE : 2 * RANGEE : 5 ***.******
*****FICHIER I RANGEE : 2 I RANGEE : 5 1*1*******
I*II*FICHIER * RANGEE : 2 * RANGEE : 5 1*11******
I****FICHIER * RANGEE : 2 * RANGEE : 5
**I**FICHIER * RANGEE : 2 I RAN GEE : 5
I**I*FICHIER I RANGEE : 2 I RANGEE : 5 11*11*****
*I*I*FICHIER * RANGEE : 2 * RANGEE : 5 *11***1***
III**FICHIER * RAHGEE : 2 * RANGEE : 5 *1********
IIII*FICHIER * RANGEE : 1
.. I RANGEE : 4 111******1
- 3 -
AD136 1*** MACH = .597 INCIDENCE = 0.00 2D C2= 2.198E-01 CORDE*CZ~ 2.819E+01 CZ= 2.337E-01 CORDE*CZ~ 1.657E+01
AD137 **** MACH = .598 INCIDENCE = e.00 NON CZ= 2.26GE-01 CORDE*C2= 2.898E+01 CZ= 2.451E-01 CORDE*CZ= 1.738E+01
AD138 **** MACH = .599 INCIDENCE = 0.00 3D(1) C2= 2.004E-01 CORDEICZ= 2.570E+01 CZ= 1.968E-01 CORDEICZ= 1.39~E+01
AD139 **** MACH = .804 INCIDENCE = 0.·00 NON C2= 2.686E-01 CORDEICZ= 3.445E+01 CZ= 4.513E-01 CORDEICZ= 3. 199E+01
AD140 +~** MACH = .804 INCIDENCE = 0.00 3D(I) CZ= 2.067E-01 CORDE*CZ= 2.651E+01 C2= 2.645E-01 CORDE*CZ= 1.876E+01
AD14i **** MACH = .804 INCIDENCE = 0.00 3D(2) CZ= 2.222E-01 CORDEICZ= 2.850E+01 r~-w~- 2.991E-01 CORDElez= 2. 120E+01
AD142 11** MACH = .598 INCIDENCE =-2.00 NON CZ= 8.875E-02 CORDEICZ= 1.138E+01 CZ= 5.611E-02 CORDE*CZ= 3.979E+00
AD143 *111 MACH CZ= 7.990E-02 C2= 4.859E-~2
AD144 *1** MACH CZ= 8.189E-02 CZ= 4.395E-02
= .598 INCIDENCE =-2.00 CORDE*CZ= 1.025E+e1 CORDE*CZ= 3.445E+00
= .596 INCIDENCE =-2.00 CORDE*CZ= 1.050E+01 CORDEICZ= 3.116E+OO
3D(I)
2D
AD145 **** MACH = .596 INCIDENCE = 2.00 2D C2= 3.687E-01 CORDE*CZ= 4.729E+01 CZ= 4.94SE-01 CORDE*CZ= 3.S0SE+01
AD146 *1** MACH C2= 3.405E-01 C2= 4.715E-01
= .594 INCIDENCE = 2.00 CORDE*C2= 4.872E+01 CORDE*C2= 4.344E+01
2D
90
*****FICHIER * F:Rt·IGEE : 1 * f~RtIGEE : 4 *i'HHH'*****
iH':HHF I CH I ER * I~RHGEE : 1 * I~RHGEE : 4 **.~*******
*****FICHIER * RRNGEE : 1 * RAHGEE : 4 **********
iHi'HHFICHIER *' I;~ANGEE : 1 * ·I':A~II~EE : 4 ********1;*
*****FICHIER * F.:At·IGEE : 1 * RAHGEE : 4
*****FICHIER * F.:ANGEE : 1 * RRt·IGEE : 4
*~;**,*'F I CH I ER *' F.:At·IGEE : 1 * RAt·IGEE : 4' *********'*
- 4 -
AD147 **** MACH = .593 INCIDENCE = 2.00 NON CZ= 3.600E-01 CORDE*CZ= 5.151E+Ol CZ= 4.740E-01 CORDE*CZ= 4.367E+el
AD148 **** t1i,CH = .594 HICIDEt'ICE = 2.013 3Dq. CZ= 3.027E-Ol CORDE*CZ= 4.332E+Ol . , CZ= 3.S61E-01 CORDE*CZ= 3.557E+01
AD149 **** MACH = .594 INCIDENCE = 0.00 2D CZ= 1.995E-01 CORDE*CZ= 2.855E+Ol CZ= 2.419E-01 CORDE*CZ= 2.228E+01
AD150 **'** MACH = .595 INCIDENCE = O.O~ NON CZ= 2.081E-01 CORDE*CZ= 2.978E+01 CZ= 2.418E-01 CORDE*CZ= 2.228E+01
R!1151 **** t'1ACH = .5'34 HICIDEtKE = ~).00 3D(1) C3= 1.865E-al CORDE*CZ= 2.669E+Ol CZ= 2.076E-Ol CORDE*CZ= 1.913E+01
AD 152 **** ~lACH CZ= 2. 25::;:E:-\) 1 CZ= :3. ::::41E-Ol
= .802 INCIDENCE = 0.1313 CORDE*CZ= 3.225E+01 CORDE*CZ= 3.078E+01
2D
AD153 **** MACH = .803 INCIDENCE = 0.00 NON CZ= 2. 400E~-OI I~JRDE*CZ= 3.434E+01 CZ= 3.755E-01· CORDE*CZ= 3.460E+01
*i~'***F I eH I ER.: AD 154 **** ~1ACH = .803 INCIDENCE = 0.00 CORDE*CZ= 2.911E+Ol CORDE*CZ= 2.788E+Ol
:3DO) * RANGEE : 1 CZ= 2.034E-01 * RANGEE : 4 CZ= 3.026E-01 ;;'''I~********
*****FICHIER * RAHGEE : 1 * RAHGEE: : 4 i·HH*****·**
*·H*,*FICHIER '* RANGEE : 1 * F:ANGEE : 4 *******~,,**
*****FICHIER * F:ANGEE : 1 * F:At·IGEE : 4 ******fHH*
AD155 **** MACH = .595 INCIDENCE =-2.00 2D CZ= 6.814E-02 CORDE*CZ= 9.751E+oa CZ= 6.321E-02 CORDE*CZ= 5.824E+OO
AD156 **** MACH = .596 INCIDENCE =-2.00 NON CZ= 7.989E-92 CORDE*CZ= 1.142E+Ol C2= 6.654E-02 CORDE*CZ= 6.l31E+oa
AD157 **'** MACH = .596 INCIDENCE --2.00 3D(1) C2= 6.874E-02 CORDE*CZ= 9.836E+e0 C2= 6. (166E··02 CORDE*CZ= 5. 5809E+00
91
;~****F I CH I ER ,~ F:A~IGE:E : 3 ,~ F:At·IGEE : 6 ,r.*********
*****FICHIER *' F:AHGEE : 3 *' F:At·IGEE : 6
*****FICHIER * F:At-lGEE : 3 *' RAt·IGEE : 6 *****~.****
*****F:rCHIER * F:At-lGEE : 3 :0,. RAHGEE : 6 **********
*****FICHIER *' F:At·IGEE : 3 * RAHGEE : 6
*****FICHIEF: *' RAt·IGEE : 3 ;0; RAt·IGEE : 6
*****FICHIER * F:At'IGEE : 3 * RAt·IGEE : 6
*****FICHIER * F:At·l(~EE : 3 * F:At·IGEE : 6
*****FICHIER * F:At'II~EE : 3 * F:A~H~EE : 6
*****FICHIER * F:ANCEE :. 3 * F:At-lCEE : 6
*****F' I CH I ER * RAtlGEE : 3 * F:AHGEE : 6
*****FICHIER * F:At·IGEE : 3 * F:AHGEE : 6
- 5 -
AD 15:3 **** t'lACH CZ= 9.48ISE-02 CZ= 2.CI7IE-'~12
AIl IS', ****' t'lACH (;Z= '? 8'?3E -£12 CZ= 2. 32:3E-'32
AD 16121 **** ~lACH CZ= ';'.454E-.n CZ= 1.742E-'Z12
= .595 INCIDENCE =-2.00 CORDE*CZ= 1.030E+01 CORDE*CZ= 1.070E+00
= .596 INCIDENCE =-2.00 CORDE*CZ= 1.074E+el CORDE*CZ= 1.200E+00
= .596 IHCIDENCE =-2.0121 CORDE*CZ= 1.026E+01 CORDE*CZ= 8.998E-el
2D
t·IOt·1
AD161 **** MACH = .S97 It-lCIDENCE = 0.0121 2D CZ= 2.537E-01 CORDE*CZ= 2.754E+01 CZ= 1.926E-01 CORDE*CZ= 9.945E+00
AD 162 **** t'lACH CZ= 2.711E-Ol CZ= 1. 9 '?::;: !;:-o 1
AD 16:3 **** t'lACH CZ= 2.4111::-01 CZ= 1.6471::-01
AD 164 **** r'lACH CZ= 2. :::4:2E-Ol CZ= ::;:.19::;:E-'jl
AD 165 **** ~lACH CZ= :3. 0::::2E-(11 C:Z= 4. 1 i.~2E-01
= .598 IHCIDEHCE = 0.00 CORDE*CZ= 2.943E+01 CORDE*CZ= 1.029E+el
= .598 INCIDENCE = 121.00 CORDE*CZ= 2.617E+01 CORDE*CZ= 8.506E+0e
= .807 INCIDENCE = 0.00 CORDE*CZ= 3.085E+Ol CORDE*CZ= 1.649E+01
= .805 INCIDENCE = 0.00 CORDE*CZ= 3.346E+01 CORDE*CZ= 2.150E+01
t·ION
:3D 0:: 1 )
AD166 **** MACH = .804 INCIDENCE = 0.08 3D(1) CZ= 2.488E-81 CORDE*CZ= 2.701E+01 CZ= 2.55SE-81 CORDE*CZ= 1.3:20E+01
AI1167 **** t'lACH = C',~,~ •• .J • • ' I He I DEt·leE = 2 •• j.) t·l0 t·l
r· ... -... .::.- 4. ::;:::::::E-(\l CORDE*CZ= 4. 76:3E+O 1 CZ= 4. ::::4:3E-'J 1 CORDE*CZ= 2.246E+Ol
AD 16:3 **?* t'lACH = .5':"':" I t·le I DEt·leE = 2.00 :3D ( 1 ) C:2= 3. 752E-'31 CORDE*CZ= 4.074E+~)1 CZ= 3.65SE-131 COF:DE*CZ= 1. :3:39E+01
AD 16'3 **** MACH = .599 I t·~c I IIEHCE =a 2.00 2I1 CZ= 4.237E-I)1 CORDE*CZ= 4.600E+e1 C2= 4.250E-I)1 CORDE*CZ= 2. 195E+01
92
Annex 2
Listing of Adaptable Wall Shapes
93
- 1 -
Listing of adaptable wall shapes (rows 2-S)
:---------------------------------------------! AItAPT.: FOF.:t'1E t'1ACH: I t·K I ItEt·KE ! ! ItEPART: 0,6 : 0,8 : ! !---------------------------------------------I ! NON :.' AIt445' : 122 : ! ! 2-D : 145 : +2!
3-D AIt'3122 : 123:: ! !-------:-------------:-----:-----:-----------1
N (I t-I : A It 4 A D4 : 1 (1;-' : 1 ° ::: : 2-D : 136 : 134 : ° 3-D :8D~10;-' AD9118: 117 : 119 : 1
!-------:-------------:-----:-----:-----------I ~~Ot·~ : AIt4 : 142 : 2-D : 144 : -2 :~:-D AD'~ 142 : 14:::: :: 1
,---------------------------------------------,
Forme depart = Beginning shape
94
F' ile: AD136 Lines of current (mm)
, N' 1-·· ..
I 2 3 4 ~
• , • ~
10 'II ,\2
Il I
'15 1\6
" II
I' 20 I Zl
22 23
I:: .. I ::5
" 2ti I I 2' I I 2& I
AbsC. tZ L 1:.H.utl~ L.r':.B •• I .... --_ ... __ I .... __ ...... __ .. 1 ............. - - .... I
-8UO 1 "'. uu U. I)u -'~4 , . U; II" .. 711.41 .101 0., -';?I). IJ • 'l~ . lot -630 4 .!i) .1":l .. S~2.1) H .4'3 .. ".;., ... ~ .~8 ... 5:2,') .~ .... 12 .. 48!?1. 'J ,.7 35 -~57.'; ."8 . J9 .. 42' , .'SIu ~u
-3!f'.:" LUof <II .... -371. 2 1. U . '411, -345.0 1 ,,~ ... ~ ... 119.f 1.... .~1 .",., 1.'~ ,'!)l .. 273.U 1. ~~ ~.2
.. 2S1. 1 .,of .,~ -~10.3· 1.''1 oS" .. 21111 l.Ll .~ .. -1"1.2 ,~o; .'l' -1:"".4 ,oIl'J •• U -lS',J ~2 .';2 .. 1"'.1i .'3 . ., j -in.s ,='2 ... 2 -12u.9 ~1 iii .. lu'l. .U .;U ... , ... '11) . j, . .,.,
I 29 -oJlJ. e~ 1)5 .~:i 30 "'~.I)~ lJ .'5.1 11 ... 'i!l 0:0 .::0 . .,11 32 "''i0.39 ." .'J?
I 13 .. 51. 3~ 3.;ot ,.; I 34 I -42.57 l . H ." I 35 I -33~!I 0103 . '55 I 36 -2'5.33 47 ')'
3" -16 94 "9 .~"'I 39 I .. >3·U . 5, ~ , 39 I VIJ . ~l ':.l
I 'ttl <U 51 . ':Ii 0111 16,j" 3. ')1 ~4 .. 2 2':0. J) J ~, ':".;
I 413 33 . a, 3. '.I . ~..: I 4.. 42.'57 1 ~\J .::.,;
4' , 1 39 J . "'i~ . '5 j 46' 61) . l~ 3 .,,~ ~.j
4' 69."iU J.~~ ~~ , 413 7'.09 3. -u S-. I ~9 o)B.~9 J JB .:4
I '0' " . Oil 1 H . ':' 1 ,~l. 109"?] 327 .~l
'2120.941 3.11J . .,.;0 '3 132.P3 .09 .~2 54 1"','56 .57 .~l ~'I 159. 13 . H 6''1 56 1'" .. 3 :'~ .• 1~ " 1'31.:3 .'57 .-,7 58 I 210.Jl .57 .1f1!o
5 !II 210 Z' ... , .4'5 '0 ;l'H.l' 2.31 .. .. 61 I '2"71 .• " 2 • 15 ... .. ';2 I 29'. ,.. 1.'9 ."" '3 I 31'.90 1.134 ~3 6.. ' ..... 98 1,'1) 43 ," 3'1. 23 1.5, . -,3 6' "S .'0 1 .041) , "1 67 "27. '" 1 .25 . )111 'I "'5'.~5 1.11 .J' U II1II1' . .." ,99 33 ~O I 5'22.01 ·8' JO
--,---- ----,---
Haut = high Bas = low
2
File: AD134 Lines of current (mm)
: ~ ~ ~ ~ ~ ~~ ~ ~~:~ ~ ~~ ~ ~ ~~ ~ ~ ~ ~~~ ~ ~ ~~ ~:~ :~~::: 1 -800.1 0 'JU IJ 'J" 1 .. ~ ... " ,Ub
j ""11." . j.J I" .... ,0.\1 .JO
0; .... JU."I . ""Ii i ,,5:;2.. .J~
., .. I)~'.I) ... :a 8 -~12.a .S< ., -,,"9.1J .• J
1'" .. ,"~._ .7 .. II -~27.~ .0"$ 12 ." .. ~., .w,
I 1l .. )'1.2 l.U I 1~ -J"'.U '.2~ I 15 t -U'.9 1.,,)
16 "295.j 1 'I' 1.' .. 2'3.0 1 .~, 18 .. ?1.: ·l.11 u .::30.3 l.u" 2. -2Ia.l 2.2' 21 ."1.2 2.II1II2 ~:! -174... 1.b'l 23 -nt'.l 2.~ .:'4 -145.6 2.1:II'J 25 -132.' lOu 26 ... lfiO.~ '.0' ~., -'u~., 1.18 4!9 .... ~~.I)tl 3.'2' '29 -lIie.tI~ .i.3~ lu .... ;O~.u:t J . .qi Jl -"9.~u J.,9 l2 -",1J.39 J.lti 33 -51.H' 3.:"9
'34 -42. " J." I 35 ... 33.39 J.'2
:iti -:5.JJ 31 .:t~ J? -lO;.~.q 4.u2
, H .. 8.011 ....... 5 I)~ OlllJ ~.o,
I 411 !oJ "'1 4."" 041 1';. Jt.. ".09
•• 1 •• 1 .~ 1
I 46 • ., , ••
1"'':1 1 50 , 'I I 5: , '3 I ~ ... , '!I'i I 'ji)
,. 59 ~" , I
'2 51 ~. '5'5 I
'" 1 .. 68 69 1
I '0 I
~!I . .JJ J3. 'J~ "2.51 51 J9 'iu H oi~ ';)tJ ":"9 Il~
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:,~19. ":"S ~~'J ':'~
1Z~. n lot'S !Iii 1'::'] ';3 17..:t "IJ 1~1 .21 210. Jl ~JO .".., 'Z51 1? '2"',) 05 2~5 ~4 319 ~o '''40 ~e 3"'1. :3 l".l~. "0 ",2;1 "6 "5~" ~,
4089.05 522 U1
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" 1
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· :,7 ..l" I
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• .:~ I
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· " .:4 .t'!l .1"'1 I
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.0-: -_._--- -----'----,
95
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File: AD144 Lines of current (mm)
..... ........... ................... __ ............... -.................. -......... N , a:lbac. ,~ L.C.Mau'\l2, to ,'; .e •• ,
: ........ 1 ..................... 1 ............... __ .. 1_-_ ................. ,
1 , .. ~OO .1 2 , ... ?54.7 , , , .. ..,11.~
I ~ , ... "0. III I ~ , -no.~ I , I ","2.It ,
-~". , f -'22. a , , -49'." ,. , .... ~,.,
:l , -427.~ :2 .. ,~ •. 7 ,3 .. )71..,
" .. 1 .. 5.(f I "
, -lit.'
" , -a'·' ., I .':'7]. u
I ;. I -2".2 I .f -;1').1
:) -:-1>1 I
-- -1t! .: I :~ -1" .... 4 I ;1 I .. .;.,~ , , :< I -tllll!o .Ii 0 " -11: .'j , a -ll!) ·1 I =7 '!:n ~ I a .. " .')8 I -, .. fa .tI' I 11 .. ,~ .U~ 0 ! ~ .... , •• ~: ... .;., .39
11 -51. I, I. .. 42.S,
" -33. a, II -:5.13
0 17 -61i .~ .. -e .. l! 0 0'0 ., ; .. . ; I< ... .: .:~ 11
I .. 3 11 .~' I .. ,2 5'
.. ! 5; ,. I •• '" 19
" H '0 .. '9 " I ., •• ~ . 0 .. , 99 · ,,4 , .. I 109. ~"J , " I 1:0
_. I ~3 u~.e3 , ,. loll, .5' I cc ,
'" 3J !6 174.43 57 "\ · ~3 I H , 213 .Jl
" 230 l~ ,~ 2" .17
I Ii ~ I 2~1 · ., I .2 I 2" .. I ~3 31'. !O I .. 1""'.'8 I .! 171.21 I .. , 39'1."0 I ", "'2? .4to I n 45'.55
U 4".05 '0 '22.01 , __ ,
Haut = high Bas = low
, U. vI) , U. ut.l , .IJ~ ". uu · .~ · .1 · ., .01
11 .~1 I I~ · .1
.U .• 1
.2' .' "0 J~ • ••
· #5 .. , ,,'2 <2 .... u4 , '0' - ,p ,. - .• ul
.0-:' - .11 79 - .It
· .. - " ," -." I o,~ - 17 1 .. ' ;, I .. -. ~s I .-;t,) - !. \ .'4 1) - .0' I ... - "'2 1 ~, - <~ I .. .-I 4:i~ - 'l I ,~ - 5~ \ " .... .,0 \. .p .;3 I · ~"" .. . 1Ij~
2 .Jo') •• I ~J ... . 71 I
:3 - N I~ .... ;-" ~2 .. c.
" .'s '. '" '" .. ••
. 31 ... to'J J:l · " ,2 · ;oq
.. d· ...... .,
.lot .;"') ,j~ .73 os .71 J~ - .~IJ
" - ~.;
)3 -,.; ~
" •• ,~ -. <;Ij -, 0 .55
" I ... ·iIl II -. "g .)~ ...
I · ~4 -."U I .97 "'. '1' 1 .90 - !< I .. ~1 -. n I · '55 .... 29 I .51; -. :!5 I ..... ... 21 \ · J~ ... L6 I .31 - Il I · ~~ ..,IJ)
\. I> .• J'j 1 .1l-.1 ' .,.~
.·rJ. .j; · b~ .17
I .,. .20 ,. .6' .23
---- ----
3
File: ADl45 Lines of current (mm)
.......... -... _ ........... -- ... -..................... -.................. _ .. I N , Abac. 1% L.C.KautIZ L ,'::'. ill •• I 1-....... -_ .... -- ........ 1- .. ----.. • .... 1 .... --- .... _ ..... I
1 -'00 .1 , 0.00 u. uu 2 -~~., , .1'41 · , . , ""11 ... .~, ~'1
~ ... "0.0 .3. · .~ , ·.JO .• I .51 . .. ..: I , -5'12.oi .. , .>0 . -~56. 5 . .. ,',
.. '22 • .~, · ~. J
-489. \J I 1. .• l 10 -.". ~ 1.17 · .. ~ 11 ,,41:1. , 1,"''' I. .0, U ",)9111,' l.ttl I .. 11 -Pi. 2 LV" 1.1'" 1~ -) .. , .0 I.t~ 1. 'J-: 15 -)19." 2.2. 1.,,)
I " -2,,5.! 2.4Z 1.11$ I 17 ... :'73 . .., 2.U 1.041) I :t -1' I. 2 2."1) I ,. I .. -21~. j 2 .•• 1 ....
2. I ":llO. J ) .1'7 1 .. :1 .. 1'11.2 l.h I " 2Z -1'''.04 l.S' L.,1
0 :1 "1!' .3 '.'S I e~ H "14~ .Ii l.*,'f 1 ' • .!
" .. 1.32.11 ".tl1 I .~ J
I ~'i "l~O ., 04.11 I .,. 0 2' -109 ? ~.21 I ... I ,e .. !o~ ~, 04. '2 I .5 ,. -.9 .s. ~."l I . .0
10 -~ .1.1' ~.'I I . .. II "09 •• 4.S0 J "I
I j:! .. 0;') · S? ~.'i • u> I 11 -51 3~ ~." 2 . ". I. .. 42 5 • ~.U · u~
I, , -13 ~. ~.~8 r.':
H I .. .!'~ .33 ~.'l IJ::"
" -tli .. ... " '.'? ~'1 -s . .0 4.'tt u. H- 0'.00 S.IJU , . 'J~ •• I Sf·""1 , ... J 0'; .. 16 .3<4 , .IJO 0: . 'i~ .2 ~';o. 'j1 , . It.., ", ., 13. ~i ,. vI)
~ , .. 57 ,. U!J , "': ., I . ~ t ,1 ... t~ 1 '.' .. ... , O;:O.JSo 4.t? 'l'J ., , " .eu 4.'1-4
49 , ".. · u~ 4. ~u
•• !. O • ... 8) · '!'~ I .0 H · ~. 4.'0 .1
.1 H H~ .73 4,'7 e. I ~~ I t: ~ · '''' lit .!!I
53 112 H ... 41 ,. ,~ 1-1'5 .'So IIt.2:=' " I " , 1'!1 31 4I.U .:''l 5. l'4.·U 1 3 .~'!l' 1."\:1 ~7 13l.23 ,. is I
I '9 I :\0.3\ J. 'u I • ~'!" ~. 230.2:' '.53 I .5J ,. ~'H.1' , J .lot I .4'!l' , H , 273. ~, 1.11 \ .-1" , '2 I 2'5 .~ ... 2.91 \ · , . • 3 31'.90 :2 .69 I ,. .. J~4.!" 2 ... , I · .~"",
I ., 1'1.'1 2.24 l.U I ., lh .,,, 2 .• 2 1.1'1 ., "17."4' 1.~1 1. uo;
•• .. ~? .!5 1.&t,) 1 IJ.i 61' "it.05 1.41 .lit:t '0 ':2 .• \ 1.;,U · .. I
'--!-- ----! -----,-----_. ---!
96
- 4 -
1
Flc'"ller ; A0142 Cotes des parols (mm)
-------------------------- ----------~l 1 Ab~c. IZ F'1.K41.lt. Z Pl. B45 1
1---·· 1---------- ---------- ----------1 1 1 -705.1) .24 -.34 1 1 2 -575.0 .66 -.72 1 3 -460.'3 1.13 -1.00
4 -355.0 1.45 -1.42 5 -275.0 1. 69 -1.70 6 -215.0 1. 76 -1.87 "7 -155,1) 1,99 -2.ll 8 -95.02 2.24 -2,13 9 -35,02 2.41 -2,40
10 :4. 9~ 2.46 -2,64 11 , 84 SI~ 2.59 -2.69 12 144.93 '2.9:2 -2.83 13 204.'33 3.0' -3.05 14 284. :0:3 3.1':1 -3.23 15 3'39 . ~'3 3.43 -3."2 16 1 S!}4 38 .3 7'; -3.8~ , ,
------._--- . -------- --------Fl.:hur : AD144
N 1 Ab~,:·. 12?-1 ;-(~'.l": 12 ?1.3o!l5 .I 1----1----------1----------1----------
1 1 -70~;.~ .37 -.21 :2 -5?~) 0 . '~/ - .70 3 -460 ,) - .33 -1 II 4 -35:; tj 2 !lSI -1 ,"1.8
5 1 - 2 ~l~) !; '2 .55 -1 ,94 6 -215 ,) 3 Jjt; -~ .28 7 1 -lS:) !) 3 4'; -2 '52 e -':5 0: 3 92 -., . :;'7 -9 -::5 ~J :1 4.'51 -3 ')6
11) 24. '~:~ '1.78 -3 .:2~ 11 ! 84. ':8 4.91 -3 ,35 12 1 l'l4 . ':06 4 91 -3 ' '18 13 204. ,?:~ 4:32 -3 .'\9 1'1 2':4:. :38 4. 7:~ -3 ,::.s 1S 389 . ~:3 4. S'* -3 ,5:i' lS 5iJ".~?:3 to! ,"' -:: 78
I I ~ I • . ---'- . ---_ ..... _---- . -------- . -----_._-- .
Fichier = File Cotes des parois =
Wall specifications Haut = High Bas = Low
Non adctpte
:l.ChH!:' : 'AD143 Cote~ ~e5 ;~rO~$ (mm'
-------------------------------------
7 1 :3 ! ':I !
"' :":
~ 1 12 13 14 !
1'5 16
-275 C -215 'J -155 oJ -':IS ,1}2 -35 c::
2-! "~O:"
3 .. 1. ~6 14-',98 ~O4.98 284 . :<'~ 3:39 .'I~ .• = '30496
2. 32 :.2 82 3 23 3 Ii> 7 '''';'s I
,';2- - 3 . ~3 ,I , 4 12 -.:i '17 4. '!t:i -.3.53 4. OS -3.~4 3 ,7~ -3.68 3 . '1:3 -3 >38 ,~ .137 -.3 . :':.2 2.34 -3,87
, I • - -_ .. - ...... - ------- -----_. ---_._- .
97
5
Flch,er : fol010" Cot •• d •• paro u ("''''')
H I Abac. 1% Pl.Haut 1% Pl.a •• ---- 1----------1----------1--........ -----1 1 I -705.0 .24 - .26 2 I -575.0 .63 -.66 3 I -~60.0 1.05 - .99 4 -3".0 1.45 -1.45 5 -275.0 1.69 -1.73 6 I -215.0 1.U -1. 89 '7 -155.0 1.99 -1. 9'4 9 -" 02 2.23 -2.13 , I -3' 02 2. <13 -2.41
1~ I H 9~ 2.50 -2 . .q6 11 I 94 99 2.79 -2. So 1~ I 1~4 9d 2 93 -2.90 11 204 99 3. J~ -3. 11 14 2-34 93 3 21 -3 . 2~ :~ 3~'~ ;9 53 -3.55 l~ 5·:4 ~'3 3. ,.:, -3 9l . , --------_. --------_. ------
__________ 1_-.... __ ----- 1 ___ ......... ____
-~:5 0 I .:3 I ... '11 -!':>'j . ~ I B -.51 .. ·H·) J 92 - 72 -3~~ .0 .71 -1 . u,i -'2":"5 .0 lu -I .12 .,:! ;p) - 1 2'; -::~ "i3: 00 -:! '- ! ~ "'i -!~ .. , 5 " .. ~";.j; .. U~ "'i ~4,9d 6 ':'2 -2 .,
'- 144 H 5 S;IJ -2 ~:;
:l ~')-t .. 5 -i .. -:: .0 -~ 2-;4 ~: .'l:! -2 ~~ . : 339 :H :g -3 . 2~. ~ : 5 1:"i 3'3 't. e~ -3 ~o
-------:' ------! -------f''="l,r ~('I!!7
~c:~., C!~S o;U'C 1S I""",)
1 ___ - • ______ ....... _1 ... ____ .. ____ 1 ____ .... ____ I
I
Fichier .-. File Cotes des parois =
Wall specifications Haut = High Bas = Low
3 ~
5 6 ?
10 :1 12 I~
1-1 :5 16
_7'.':. 0 -5"~ 0 .. ~£ .: 'J -3~ , 0 .. 2:-~ J -2.5 0 -1,!5 .0 -ii'S .Il::! -35 ~2 2~ .93 3~.~9
lH.fl ~04. '9 2H . ~ 3 3f~ . ~1 5(4 ~a
-----
... ~ I - 2S
.12 .. -. 'Ii 1. ~6 -I 00 1 3'i -I. 25
31 -I 51i 2 e" -2 0::-3 . :13 -2 :ti 3. 51 .. 2. ,-:: 3 ~9 -3 H 3 ;0<1 -3 .;00 3 45 -~ 14 3.03 -4 .63 :. ~? -5. !l I. ~5 -5 .~o
. ~6 -6 .4? - .5d ... :"" H
Non adapte
2-D
3-D
98
6
henlOr , AD122
1 H 1 Aboc. 1% PI.H ... ~ 1% '1 .••• 1 ----1--------··- 1 __________ 1 __________ 1
1 1 -705 . 0 1 I." 1 ." 1 2 1 -57'J. 0 1 J . 15 1 1.10 I 3 -"'0.0 1 4.55 1 2.30 1 'I -'55.' I s.n I 2.U 1 5 -27'J. 0 1 , .70 I ,. 'I' 6 -215.0 I 7. 4Z I 3.7' ., -155.0 I 8.05 4.11 8 -95.02 I 8.70 4.33 9 -35.02 j. 52 4.93
10 24.98 10.22 5.0J II 84.59 10.96 5.44 12 14'1.9i 11.58 5.~7 13 204.99 ! 2.29 6. !l 14 2t4.!$ \3.'25 ~.6' 15 !It.fa !4 .• 7 7.21 !6 594 ... 9 1'.';, 7 ;: , , , -----._---_._---_.
F:.ch:..!, ~t.'14~ Cot •• ~.s ;'&:C:'l (~m)
" I Absc . IZ Pl !-: .. <.;t I~ Pl.2&. 1 ......... _! ---- ..... _~. __ 1 ... - -_ ..... - ......... 1 .. _ ... _ .. _____ I
-':"~! .'J . .s .. )" .. !?15 .0 ~,) .... 'J,;
l I ~4'0 0 l. .... :;:lo 'I -1" Q :i - .2; ,5 , -z" !I 4. 19 -. :~ • -Zl'! 0 4 -:~ .23
-l~5 .0 ~~ 2" -95 . O·~ • "U " ~
~ I -35. O~ , ~O - l4
Ie I ~4.9!j ,. 4~:' -.5; I li- I IJ!4.fa 7.44 .... '; i I I: 144H ., ." -1 .';:"'t .... I ~O ... -:9 ;, .15'5
1'; 2S~.9~ 3~ -1 . .,.) I' , 3·1g.91! ~5 -~ .!oj I~ I 504.9a 3,) - '1: , ,
----------"---------- ---------Flchler : ~Ol~3
Cot •• d •• ~.:'~~I '""m)
, ~ I ,:os::. I: Pl.!'(sl.:.t IZ?l : ... I 1----: --- .. ------,- .. ________ 1 ____ ........ ___ I
""\l~. 0 1. ,e ~~ 2 -5;~ .0 3.13 I .62 1 ,
-~~ Q. 0 ~ .5~ 2 3~ .. , -S-S5. a ~. 02 l ~;t , -27~ 9 '.12 1. '::3 6 -215 .• • .03 ) J~ , -15'.9 I.U 3.50 • -'5.02 t.7" l.5Q , -35.02 10.16 3. ~o
10 2 ... f8 10.41 :2 .~~ 11 .... ,. 10.10 '2 .~, ., 1:! 1~4. '9 of .9l 2 4. 13 , 204. ~8 3.H , ~ . ~:-H , 2'<1. ~8 :3 . .;~ ., 1. ~: 15 389. i'~ 7.50 I 1. u~
I 1~ , 51)4.')& , .55 I . '5 " , . --'---~--.. '- !_-----,
F'ichier = File Cotes des parois =
Wall specifications Haut = High Bas = I~ow
Non adapte'
2-D
3 -0
99
Fichier .- File
7
hel".r : ADlaS Cate" 4 •• parol. (ftIfII)
I N lAb... IZ Pl.Haut IZ Pl. ... 1----1------____ 1 __________ ----------1 1 -'05 . ° I .21 - .2' I 2 -57$.0 1 .n -.U I 3 -450.0 I 1.04 -.It
4 .,,, .• I 1.46 .1.45 5 -27$.0 1 1.5' -1.'" • -215.0 I 1.S9 -1.88 , -1$5.' 1 1.9' -1.94 • -n. 02 1 2. 2Z -2. 13 , -35.02 I 2.43 -2.4a
10 2".98 1 2 50 -2.46 11 84.~8 I 2.79 -2.P 12 144.9'1 1 2.aZ -2.89 13 204.9a 3.aa -3 11 14 2~".99 l.B -3.2' 15 399.~'l 351 -;.~5 16 504.H 40') -3 .• ! ! __ 1 _____ ! ... ________ , ____ ,
"1.l!:h:'.fr .:ot' .. .!"t CO~4l. :tes ?.\r:l:" 'la1ft,
N I Ab.~. I;':?l !ot."u-:. I: Pi =a, 1- ........ 1-----... - ................................ ! .................. _ .... I I l' .. '05. I) 4"': .... :~
I I
I I
2 I -'7!.(I ;:! _.~~
l -460 0 33 -.'7 4 -355.0 .~2 .. 1 !l9 ~ I -275 .. ) .• 5 -1 .• 0 ~ -215.0 4 0: -: H '7 -153.') ~ ~3 -:J $ -9~ 02 ~ .. H ,
la 11 l~ 13 I
14 15 I
1~
N I
... 1' .~:: 2'\. ie !4 93
1-l4.-:'1 20<4. ~3 294 9~ 3n.~9
'0 ... 9>3
!3 .44 .5" ., . 01 74 55 47
-2 -2 -2 -3 -! -3
.9 ~3
~8 .oii H ~3 40 .il ______ I _~ _______ ! ____ _
ItlC:~U!" ':'0119 Cot ... c~s ,._:-0:'. ,""',
Abs':. '2 P1 M .. ·.lt 12 Pl.S .. u I ... ---, .... _----_ .. - 1---..................... .:._-------- I
1 -,a5 a .4oj -.51 2 -575 .• J .57 ... . e~ ] -~~o a 1.4~ -1 39 4 -3~5 • Q "2. O~ -! ,,~ , -~75 . ~ 2.53 .~. 33 , -215 0 ].01 -2 .• ~ , -1". a 3 .14 -J .36 8 -".02 4.11 -l.ts 9 -35.02 ".'1 -4.52
1~ 24.99 ".U -".H 11 84.93 4.2'. -,.U 12 144. ge , .. , -, .~o !3 204.'19 3 .• ). -li.11 H 2~4. 93 2.3' .. ';,71
l' sa9. ~e 1,21i -1 .0 is ,.~. 99 .45 .9 .b~ , ---'------
Cotes des parois = Wall specifications
Haut = High Bas = Low
I M= 0.8 I 0(= 0 0
Non odepte
2-D
3-D
100
Annex 3
Listing of Test Files
101
Key to Annex 3
Fichier ::: File Parois rectilingues = Rectilinear walls Symetriques = Symmetrical
Page format:
MACH HIGH AND LOW WALLS MACH LATERAL WALLS AS07 WING
I HIGH LOW I HIGH I~OW I MACH I MACH I MACH
DBL. RECORDERS UPSTM PTHOLE
LFT. LAT. RECORDERS
DNSTRM PTHOLE RT. PTHOLE
RT. LAT. RECORDERS
LFT. P'fHOLE
NECK RECORDERS
102
1
LISTE DES ESSAIS "AILE AS07"
~**~.~~~~~~*~*~~~~*~~~~~;;~*~~~~***~~*~+*.~+~~*~~~~~~~~++~~.~~~-+~~++~~~-
;; FICHIER AD4 PAROIS RECTILICNES DIVERGENTES 4 '+ ADH"5 IDEM + ROTATIIJN DE 30' 0.: ',iER:3 LE HAUT) 4 ;; AD___ : FICHIER DE L'ESSAI N 8___ .. ;; AD9 ____ : CALCUL 3-D DE LA NOUVELLE POSITION DES PAPOIS ~~+*~~~*,**~*~~~~~~~~+~~;;~~~~~~~~~++**~**~~~*~~***~~*~+~*~+~~~~*~~~+~~+~
**~*~****.*~**+~~*~+~~~~**~*~~*+.**~~~+~~***~~~~*~~~**.~~~+.~*~~ ;; ! Hle.! R~1NC;EE:3 ! FICHIER ! ROT, ! ! ~18. "" ;;FICHIER!AFF. !MACH DE PRISES!DE DE?ARTIPAROIS! ADAPT, !D'ITER.'+ *~*~~.~~!*~*~!+~+. ~+~~~~~*~!~~~~*~~~~!~~~+~~!~~~.~+~!.*~~+~~+ ;; ADL0~ a ,,' .! ~ ! AD4 ! 0 ! NON 1" ;; ADHli ~) .6 ! ! 0 ! 1 .. ;; AD !lilS 0 ,:3 ! 0 1 ,. ;; ADLl0 -2 .7 0 1 .. ;; ADll~ 0 7 AD910~ 0 !3-D <1\! 1 ;; ;; AD11'; 0 .1 AD'Hl~ a 13-0 <.2:'! 1 ;; ;; ADl17 a .6 AD91a7 0 3-D I 1 ;; ;; AD118 a .8 AD910a a 3-D (1)1 .1 ;; ;; AD11'3 til .:3 AD'Hl:3! a 3-D (1)1 '1 .. ;; AD LN ! +2 ! • ~ AD4 a ~jON! 1 ;; ;; AD121 !+1.~1 .6 AD44~ 30' NON! 1 '+ ;; AD123 1+1.'5! .6 AD9122 30' 3-D 1;; ;; AD1Z4 !+1.5! ., AD44~ 313' NON 1;; ;; ADL2'5 ! +1. '5! • i AD91N 30' 3-D 1 .. ;; AD126 ! +1. ~! .:3 AD44'5 30' NO~l 1;; ;; AD127 1+1.5! .:3 AD"lZ"3~)' :3-D (1)1 1 ,;. ;; AD12S ! +1. '5! .:3 AO'?127 30' 3-D (Z>! 1 ;; ;; AD1Z': I +1. ~ I .:3 AO'H.2S 30'3-D 0> 1 ;; ;; AD130 '·1.'5! - AD4 a 2-D 4;; "" AD131 !+1.~.1 .6 ~ AD130 a Z-D .. '" '" AD133! ')!.:3 AD4 a 2-D J. 't ;; AD134 0! .:3 AD133 ra 2-D 4 .. ;; AD 135 ~)!. 1 AD 13J. a 2-D 4 ~ .. AD136! ~! • .; AD1Z5 <a 2-D 4" ;; AD 137 ! -I). ~! ." A04453 1)' ~11~~j 1" .. AD13:3 !-').5! ." AD'?1:37 3:a' ·3-D 1 '+ ;; AD13'~ !-.).~! .:3 AD44~ 3~)' ~jml 1 '+ ;; AD14,) !-1).'5 1 .:3 AD'?l3': 'N' !:3-D <1:' 1 .. .. AD141 !-a.'3! .:3 AD'H4a 3~)' !3-D (2) 1 ;; ;; AD142 -2 ." I AD4 a NON 1;; ;; AD1J.3 -1!.6 AD91"Z 03-D 1 '" ;; AD144 -Z!. 6 AD13"·<a 2-D J." '+ AD145 +2!.~ ADDl I)! 1-0 4 '" ;;------- ----!----!---------!--------- ------1------- _______ ~ ;; AD14" +2 I • .; I 4! AD145 a 1-D 4 .. "AD14, +1.~! ." ADJ.4'5 3,)' N'~tj 1 .. ,;. AD14:3 +1.~! ." AD'?(2231)' 3-D 1" ;; AD1J.'~ 0!.6 AD1:36 I) 1-D 4'" "AD150 0 I ." AD4 a tjl~t'l 1 '+ ;; AD151 a .6 AD'(1)7 0 3-D 1 .. ;; AD152 0 .S AD134 a 2-D 4 .. .. AD153 I) .8 AD4 ~ HON ~ ;; AD154 0 .8 AD9118 0 3-D 1" ;; AD155 -2 .6 AD144 I) 2-D 4" ;; AD156 -Z .6 AD4 0 NON 1 .. "" AD157 -Z .6 AD9142 0 I 3-D 1 .. ~------- ----!----!-_ .. _----- ---------!------!-------!-------+ ;; ADl~3 -2 .6 3 - ~ AD1J.4 0 2-D I 4 .,. ;; AD159 -2 .~ AD4 a NON 1" ~ AD160 -2 .6 AD9142 0 3-D 1 ,;. AD161 0 ." AD136 a 1-D 4 .. ADl6Z a .S AD4 til NOH 1 ;; ADl63 Q .~ AD9197 0 3-D 1 ;; AD164 e .8 AD134 0 Z-D 4 ;; AD165 e .8 AD4 Q NOH 1 ;; AD-lo6 0 .:3 AD',11:3 a 3-D 1 "AD"l';; .1.'! .6 ADH'5 3.)' ~ION 1 '" AD16:3 +1.'5! .~ AD?lZ:; 30'3-D 1 ,. AD16'~ +1!. ~ AD145 Ii) 2-D 4
2
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58
TIV=299.6 K ~IV= lS5? MB
MACH ~AROIS HAUTE ET BASSE MACH PAROIS LATE~.
HAUT
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HI,IH r'1ACH
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MACH PAROIS HAUTE ET BASSE MACH PAROIS LATER.
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'I :3 Ll
33 34 35 36
~4 '55 '5';
,57 '58
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MACH DE REFERENCE= .8Q5~ TI'./=2'~'? '? K .
UINF= 231.108 M-S PI',/= 1~51 r'18
MACH PARors HRUTE ET BASSE * MACH PARors L~TER.
HAIJT
• :320 • :31 " • :312 • :31)5 • ,31)1 • :::~:3 · :301 • :3e~ • :31):3 • :30:3 • :305 • :3132 · :304 • :3~)4 • :305 .:3~H
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• 7'~9 .n'5 • 7,,13 .7'32 "I~'~I
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• 7":~ • 79:3 • 7"1) ~~~
• (I.
HAIJT
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• 8~) I • :313'5 • .~1J7 · :,07 • :3134 · i8':
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• :3·)2 • :31 I) • :312 • :~~j~ • :~e2 • :3137 I ~302
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7
• :304 • :302 • :301 .;3132 • :31313 • :3130 • ,300 .:Nl • ,3130
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4 '5 6 -,
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• ::,138 I ~'3(
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• .34;3 • ·31'5, .? ::6 .~:31
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MACH PAROIS HAUTE ET BASSE MACH PAROIS LATER.
HAIJT HAIJT f'lACH MACH ..;.
• :31', .7"'S .:3~1
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• ~36Q · '?42 · '~:36
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• :384 • ·3~J7 .304 .300 .381 ~"4
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MACH DE REFERENCE= .80:3 TI',/=.2"". '3 K
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• PRISES DOUBLES ..;. HUB. AMNT
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MACH DE REFERENCE- .6019 TI"/-2"6.4 K
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27
MACH DE REFE~ENCE~ .S~85 TI',/=:,2"7.1 K
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1 • ,)~j~) • ?:31 ,9~7 .';.44 · ,4', · :::";~ .? '5( • ?-+ 7 , :3'? 1 • :3·,r3 , :~21'5 .411)
1. '52'3 1. 4'54 1 • ;:3~) 1,26"; 1 • ')\.0)5 1. 1)2', 1.")'5") 1 . ~)2'? 1. 1)(1:3 1.1)91)
, ·'5'? .:. ,~
•• _I
.?21 • '? 12 · :349 • ,?O~ • :3:3~
---------);2S
.. ,---------------_ ...
24
******** •• ~.**~*** • .,,*.* •• ~~*.. FICHtER AD135 N~CIT)~ 4 22/ 8/8~ 9H30 AS07 Ms.? I=0 R 2-5 ADAPTE ZD AD13~ De~ AD134 4' ITE -----------------~--------.--------------------------------------------------l'IACH DE REFERENCE= • ;'\)21' IJHIF= 231.11ilS 1'1.·:, -.
TIV=297.l K prv= 1521 Me *~~******~~***~***~~~~~*~*******~~****~**~***~*~~****~~***~*~~~~~*~~~~~~~~~~~i
.2 3 4 '5 6 {'
9 '~
1~ 11 12 13 14 1~ 16 17 19 19 20 21 22 23 24 2~ 2'; 2, 29 2'~ 30 31 ·32 '33 :34 3~ '36 .~~
~ (
3:3 '3'3 40 H 42 43 44 4'5 46 47 4:3 49 50 '51 '32 ~ ... J.j
54 55 ~.; ..... .J(
58
MACH PARors HAUTE ET BASSE ~ MACH PAROIS LATER. '" A I L.S H~~?
HAIJT
.70:3
.704 • 7'~:3 • (1)0 • 6'~'3 · 7'~n • (1) 1 • (~2 · 7~)2 .704 • 7~J2 .699 .701 .701 • (1) 1 .701 • (1) 1 .704 .704 • (~7 .706 .7\.j7 .7~7 .(~6
• 7~:3 • 7~:3 .714 o (1'; .721 .71 :3 .7~2 .717 .71'3 .714 .71'5 • :"14 .717 .717 .721 .11:3 .71:3 .713 .71:3 • :-(\3 .:-06 .;'0'5 • (1)'? .7Q'? • (1)9 • (1)'5 • (1)4 .104 .(1)4 .-:-133 • 7~:3 .700 · ';',7 • t5';'2
8AS
• (1)1) .(1)4
.702
.702 • 7~3 .N4 .7132 .(01)
HAIJT
* PRISES DOUBLES
BAS * '" '" * * S'~
• ~0 • 61
.701
.(1)0
.7~1 '" ~ '" ~
." P~ISES LAT. GAUCHES_
~1ACH
HU8. A110~lT
1 2 :3 4 5 6 7 :3 '?
10 11
.;'013 • 69'? • 6'~'? .700 .69:3 • 6'~:3 .~9a .697 .698 .69:3 .699
1'1ACH •
.~02
.~~2
.7'102
.7133
.704
.704 ,7e, .;'01 .700
., '" '1·) .. 11 • 12
• (1)2 .0',7 .697 .6'?9 .I'H:3 .700 .71n .702 .7~2 .0'?9
.7131
.7'1)1
.704 • 7~Jo .;'1)3 .;'13 .7'HI ; 710 .715 .707
HUB. A"/AL HIJ8. DRO IT •
13 14 15 16 1;' 1:3 1 'i1 20 21
• 0'?:3 • (1)1) .7~1 .701 .71313 • ';'?9
7:3 .• 7'J3
.6';'5 ;:
• PRISE! LAT. DROITES*
74 ;''5 7~ 77
.7,)4
.7'03 • 6'~7
;+
*' ~
. ., .. '3 4 '5 6 7 :3 .,
10 11
7 :3 .? • o';'~
.6';';
.0'?9
.713:3
.7(14*
.704
.701
.7~4
.7'34
.701
.701
.701
• ~.~7' .0·?9 .6·?5 · ';'~', .7CJ1 .6'?:3 .6 ?:3 .7'01 .7.)4 .7(1:3 .~~2 .700 · ~"'~ .;'~1 .703 .701
• HU8. I~MUCHE
1~ 11 12 13 14 1S 1'; 17 1 :3 1 '~ 21) 21 • (131)
.7~13
.71313 • 7~~) .7~1) .7~13 .701 .7'32 .7131 .792 .71J0 .701 • 71J~ .7CJ13 .701 .7131 .7132 .(1)13 .~99 .697 • 096 ,';97
.725
.71 :3 • ;',)9 • :-:;,19 .;'02 • ;'1)4 .701 .0'?'3
.;'5:5 • ;""39 • .~~:3 • '?26
1. Ij ';' 2
• ~,?,~ • ;',)0
• 6'~:3 .6?'5
1. 146 1.0913
• :363 .. .... · (~(' · 711
.1
7 :3 ';
10 11 12 1'3 14 15 16 17 1 :3 1 " 213 21 '':1"') .. -* Z:3
• 24 .. 2'3 ;+ 26 * 27 * ;::s ... ;29 * :3~ .. :31
.711 • ;'11 • 710 .71a4 • 71)'5 .7~7 .710 .712 .71·'3 .711 • ;'1 I) · 70~ • 7'J:~ • ;'0:3 .7'34 • ~:a3 • 7~4 .704
31
.;'1;)4
.70434
.70'3 .35
.70'336
.;'04
.7'0:3
.710
.712
.714
.711
.707
.700
.105
.;'02
.7CJ2
.;'02
.7~2
.7'02
.702 17~2 .~~~ .70:; .;'02 .7'~2 .7~2 .~~2 .701 .~'3:2 • 7'('~
.7C~
.702
.:-02
.7'IJ2 • 7'"~j2 .;'01 .:-031 .;'001 .7'»1 .71) 1 .701 .701 .;'1)2 .:-az .i~2
• 7~)2 .7~2 .7'"0:2 .702 .~02 • 7~):2 .702 • ;-~J2 .702 .7'"02 • ~1J2
24
• ~7~ .I£·3'~ • ;'42 • 3Ij,) .7'3( · ~~~ · ~~~ ·~H , ~:3~
1. ():::3 1 • ;j5~
• '?'3S • :3:37 • :3:-~ • :35:3 • :3~'5 • ,3"2 • :,4) • :3:3:3 • :335 • .321 · :~ I '5 • :383 • ~57 · ~:~~ • ;";:3 .;'% • :"'?2 • 7'5, • ;"2'5 · ~~7 • ~'5:3
1 • l?.s 1 • ~)~~
• '?22 • ,~'?4 • :::3~ • '3;"? • '~~? • ·::5'; .::4~ .:33:3 • :32'3 • :312 • ;"'?3 • 7'?,) • ;':31 • ~4:3 --.. • I I I
/26
2S
*.~*.*.*.* •• .;.**.**.~.;. ••••• *... FICHIER AD136 N~(IT)3 4 2Z/ 8/85 'H55 A907 Mm.S I30 R 2-5 ADAPTE 2D AD136 D!~ AD13S 4' IrE ------------------------------------------------------------------------------
3 4 " . .)
~
:::3 ··3'~ 410) 41 42 4:3 44 45 46 47 48 43 '39 51 52 53 54 55 56 5, 58
MACH DE REFERENCE= .5972 TI ' .... =295.:3 1<
UINF3 231.l9a M,! PI""3 1:39:3 MS
MACH PAROIS HAUTE ET BASSE .;. MACH PAROIS LATER.
HAUT
.S"S
.'39S .5',', • ~"S • 5',:3 · 5'", ',5,,7 .597 .5n .5,,8 .5,,7 • S'~05 .597 .5,,6 .5,,6 .5% • 5'~7 .5';';& .5';8 .5',', .699 .610)2 .693 .692 .69:3 .692 .695 .695 .69:3 .696 .698 .696 .~e7 .69'3 .696 .610)05 .697 .~96 .6110) .698 .69S .610)'3 .1')~7' .604 .69:3 .602 .602 .601 .60e .5,,8 .5,,8 • ~',7 • 5'~7 .597 .5',7 .5% · s',s .597
9AS
.5',6 · 5'~', .5',:3 .5',:3 .5',8 .5'n .~97 .536 .5'n .5,,4 .5,,6 .5',05 • S',05 .5305 .'3% .5',4 .5,,5 .S"S • 5',05 • 5'" .s'n .5,,4 .5'3:3 .5',5 .5,,6 .5% .5% .5',:3 .5,,:3 .5',8 .5',6 .5',', · S',', .5',7 .5,,7 · ~',8 • ~',6 .5,,6 .59'3 · S',5 .5','3 .5,,5 • ~',6 .5',05 .5305
'. s'n .~% .5% .535 .5',5 .5',5 • S',6 • 'S',6 .S"S .~34 .594 .5'34 .S'?8
HAUT MACH
* PRISES DOUBLES "' HUS. AMONT
5', .;. 60
61
.5',7
.5',8
.5',6
* ~ PPISES LAT. GAUCHES*
· 5'~:3 • S',8 • ~5'?" · ~~'?9 .609 .692 .692 · ';;92 .6es .600 • ·S'37 .594
.5'?:3 .5',',
.5',7
.5%
.595
.5',:3
.5',8
.5',:3
.5','3
.5'3'; • ~.?t5 • 5'3:3
.;
.;. PRISE! LAT. DROITES*
.59'
.5',7
.5'?7 • 'S'?6 .5',6
HUB. AVAL
:3
1 ~) 11
.5',:3
.5,,:3
.597
.598
.597
.5'37
.597
.598
.59:3
.5',6
.'5%
• ·S'~7 .694 .606 . .695 .69', .612 .613 .619 .6S" .6e9 .614 .~08 .604 .~92 .5'37
• 5','? .5',7 .5'?..\ • 5'~4 .S'?2 .5'32 .5?5 .59:3 .S'N .5',6 .5'?8
.;. HUB. GAUCHE
~
• 'S'?:3 .5',5 .5n
5'~o:.
,5'38 .5·38 • S'?6 .5',5 • 5'~5 • S'~6 .5',6 .5';'5 .5,,4 .5,,5 .5',:3
PP.I3ES COL
• !~52 • ,5';',; • :-,? 1 · :35'(
1. iH'~
1.J41 • '?23 • aloJ 1 .6'?4 · ;,32
.;.
3 4 '5 6 .. , :~ ':'
10 11 12 1 :3 14 15 16 17 1 :3 I'? 20 21 22 2:3 24 2~ 26 27
.6~3
.602
.6032
.539
.599
.';~9
.6@2
.604
.694
.604
.6032
.602
.601 • 6~J0 .538 .53~ .'597 .5',7 .597 .598 .5',:3 • 'S',9 .5',7 .608 .601 .602 .604 .605 .~0:3 .~01 .609 .598
NACH •
HUB. DROIT ;;.
:3 4 5 6 7'
.598
:3 ';:I
10 11 12 13 14 15 16 17 1 :3 1 " 20 21
.59:3
.S9:3
.5',8
.59:3
.59:3
.598
.5,,:3
.59:3
.'598
.5,:3
.5,,:3
.5.,:3
.597 • 5'~7 .597 .'5'37 .597 .597 .5';';.' .S~( .597 .597 .5'37 .597 • 5'~( .597 .5',:3 .5 ?:3 · S'37 .5'"
,. . 28 ,. 2',
• 5,,:3 • 5',:3 • 5',:3 • 5',:3 • 59:3 • 53:3
3:3 .597 * :3':' .5':7 :+ 40 .5',7.;. 41 .597 .. 42 .597.;. 4:3 .597.;. 44 .597" 45 .5',7 ,.
t'lACH
, St5', .5:33 .61'3 .6:39 ,1:)7':3 .642 .':;91 '.5:34 , .,,~
• ~.~IJ
• :3:31 • :3:35 • :"6? .7:3:3 .~24 .715 • ;"LJ5 .701 .701 .6% .6,3 • ,-5:3:3 .05:30 .~71 .55';' .5";:3 .~24-.tE7"'l .664 • ~:35 .';11:) .5'?5 .3PJ • '~3'~ · ~'~;.' .7"5:3 • 7"4~)
-. .., ... ., ..;"
.;"21 • 711 · (~:3 • ';';':3 • ~'~2 .6:30 · ~~.? .~r5'; • r55:3 • ';:3~3 .0S7' ,"£24
/27
26
~~~~~~***~*~*****~*~*~~*~~*~** FICHIER AD137 ~~~(IT)= 1 22/ a/a~ 10H25 AS07 M:.~ I=0·-30'+ROT.3a') R 2-5 NON ADAPTE AD137 DE AD44' l' ITE PAROI:3 RECTILIr:itlE:5 +30' -------~~CH-DE-REFERE~CE:-~597;------~I~F:--;;~~~es-~~s----------------------·
TIV=3131.0 K PIV2 1393 MB *~***~**********~*~~~~**~~****~*~~*+~~~*~~.~*~**~~*~~~~~~~*~~~~~~~*~~~~~~~~."
.. , ,3 "
1 ~) 11 1Z 13 14 15 16 17 1 :3 1'? 213 21 22 23 24 2S 26 . .,~ ... ,
MACH PAROIS HAUTE ET 9ASSE
HAUT
.605
.61H
.6131
. 597
.595
.5'?8
.5',;" • 5',8 • 5',:3 .5',:3 .5% .594 .5',5 · 5',6 • 5',;" • 5',:3 S'~':'
SAS
.S'H
.5',5 · S',,, • 597 .599 .61313 .~97 .5',7 .59:3 .S95 .S'?6 · S',,, .59~ • S',7 .59:3 .5',7 .59:3 • S'?', .59', .05013
HAUT
• PRISES DOU8LES
.'S'"
.598 • 'S',7
.5'?8 .. ,~ .. • ·oJ ~ I
.601 • • PRISES LAT. GAUCHES.
72 7'3
.5,,9 • 60~) ,~i02 .613:3 .6Ij', .613 .614 .614 .614 .~~? .602 .5;-8
• .s'?7 .601 .61)2 .61313 .59', .6136 .6134 • 604 • 6~:3 .6032 .~~4 .6t16
* • PRI3ES LAT. DROITES*
74 75 76 77
.61313 · ;'?7 .5',:3 .5',7 • ·S'?9
· 5 ?:~
MACH PAROIS LATER.
HUB. AMO~lT
2 3 4 5 6
:3 '?
10 11
.5"',
.~99 • .59';& .'3'?8 • ~9:3 • 5'~8 .59:3 .~9S · ~',;" • 5',:3 .S9:3
HUB. AIIAL
4 5 6 .. I
:3
10 11
.6131 · 6~2 .602 .6;):: .6'32 .';02 .6~2 .~03 .~04 · 6~j2 .602
r1ACH •
:3:3 • ~~5 -+ 34 .617)4'" :35 .6'j4 * .36 • r5~3 .. :3, .1'517):3 • 3:3 .603.;. :3', • ';~3 .; 40 .6134 ., 41 .6134., 42 • 60~ * H .6iJ3 '" 44 • 6132 '" 4'5 .601 ..,
HUB. DROIT .,
.2 • 59'? ~ :3 • 5'~', ~ 4 .5',:3 .;. 5 .5'?:3 :0-
6 .5',:3 • "( .59:3 * :3 .59:3 ;(-'? .5',8 ;-
113 .59:3., 11 .59:3" 12 .5',8 .,
.602
.1'5132
.613:3 • o~):3 .1'50;" .611il .611 .612 .612 .615 .616 .61 :3 .617 ,I'jZl .61:3 .61';0
• QO~) .600 .59', .600 ,.59'? .6013 .6013 .60:3 .60S .605 .603 .606 .604 .61()2 .602 .603 .601 .601 .601' • .6013 .601 .601 .6133 .604 .60:3 .613:3 .601 .601 .6131 .6132 .602 .6131 .tS~2 .602 .602 .602
• 6J 1 .613:3 .614 .61'5 · 61:3 .623 .~24 .623 .621 ,';21 .623 .~17 .611 .6139 .~iJ1 • ';'Q2 .5'?5
.5'?7
.5'?6 • .5';'7" .5'?'7 • HUB. GAUCHE 1:3 • :9:3 +
• ~ 17 • 1'51', .61 :3 .61" .1'517 • 61', .616 .1'516 .616 • 614 • 1'511 .6113 • 613', .~13,? .606 .61)4 .601 .601 .s'?'? .5':( · S',5 .592 .58;" .5813 .572
. 604
.60:3
.665 · 6'?~ · :301
1. ~27
• 5'~'? • 60~) .s'?'? .6031 .6as ." .6J5 • ";~:15 • ~ ~J:3 .6031 .601 • ~~):3 .6.£I~ .602 • 6~)t 1~~1 .61;'6 .60~
1 • 1)6 • '~~J
",,~ ., .
z . ,3
1 'J 11 12 13 14 15 16 1'7 1 :~ 19 213 21
.612
.612
.612
.606
.,;~.;
.60:3
.618
.612 ,";12-.611 .610 .0510 .6'J';' • 6~:3 .6~4 • ,';~:3 · ';.3:3 .684 .604 .605 .617)5 .~;)5
.604
.0'37'
.60:,
.6a'?
.0511
.611
.05 1 Ij
.6J:3
.~06
.6(l6
14 .59S ~,
15 .5';':3 " 16 .59:3" 17 .5'?:' 1:3 ,5'~:3 1', .5',:3 2~J • ·5',:3 21 .~'?7' 22 .5':7" 2'3 • 'S'?7
~,~
- 0'
35
.5';'('
.597'
.5'3:3
.5,,:3 ,5',-:' .:; ?::: , .5'~:3 .5',:3 ,5'3:3 , 5'~:3 ,5'3::: .5'3:3 .59:3 • 'S',:3 • ::-;H3 .5'?:3 .5'3:3 .5'?:3 .5',:3 .5',:3 ,5'?:3 .5',:3
'3 4 5 6
10 11 12 13 14 15 is 1:" , " l.':"
1'" 28 21
,N
') , -'=' ., .. -' .,:,,=, -"
:' ~ ~ : ,~~; , ~:~~ , ~;3 ~ t ~~'~ .':.j7" · :- ~ ~ , ~'3;~ · ~:~:~ • ,~-l:~ • ;o-l · ;- ~~ ~~ .
• , j;; -~, · -. ~, , : :'~):3 • 7'~j:3 .783
• r5~ ~ , ,-£..1 ~ .0:) lJ , ~'?'3 • 31 ~ · ·.~~2 • 312
• ;"' .. ? ...... .., • I";' ........... • I ;,
.7?1 · - 2~; · ~l; · :"~);-· ;".): , ';:,::3 · .::~~ • ~7"J ,,:>,=,Ij
.rSJ..l ,':r5'; .-:..; .. )
2-7
*"'++++ ••• + •• "' ••• "'+."'."' •••••• +* FICHIER AD139 N~(IT'~ I 22/ 8/~~ laH4~ AS~7 M·.~ I~0(-3a'.ROT.30') R 2-~ ADAPTE 3D ADIJ8 DE AD'?!:3? l' ITE ------------------------_ .. --------------------------------------------_.-------
MACH DE REFERENCE~ .5985 TI'/=:l~O. ~ K
UINF~ 231.1~8 M/S PIV~ 1392 ~!9
MACH PARors HAUTE ET SASSE ;I, MACH PAROIS LATER.
7
HAIJT
.15015
.6~5
.~~1
.5',7 • 5',~ .5'" • 5'" • 5'3:3 · 5'?9 .6~0 .59:3 .5'37 .'5',9 .15~~ .';0~ .6~~ .5',9 .5',9 .5',9 • 6~2 .6~1 ,,;e2 .6~2 .6~3 .6015 .6~5 • 6~)7 .607 • ~YJ8 .606 .6~9 .607 .6~8 .6~6 .6~7 .-5136 .-50, • 6~37 .611-) • 6~'~ • ~'J';' · 6~', .6~7 · 6~4 .6133 .~a2 .6134 .-5'.14 .6134 .602 .-502 .15130 .6131 · 6.)~ .6')0 .5',7 .5'H .589
--
SAS
.5'?1
.595 · ~',5 .5'37 .5',9 .6~1 · 5'~', .5'", .6'.11 .597 .597 .597 .597 .599 • 5',9 • 5','~ • 60-J .6a~ .6~~ .602 .60-) .597 • 5'36 .6ao .613:3 .602 .602 .6a~ .601 .601 .59:3 .6~2 .602 .6131 .6~1 .6'.11 .600 .6013 .61313 .6013 .599 .5','3 .5'?8 .5'~:3 .598 .599 .601 .602 .501 .61313 .'59'? .598 .6~1 .6·)2 .602 .6,)2 .6133 .6'.1S
-
;I,
HAUT MACH
PR I :~ES DOUBLES ;<, HUS. A~!ONT
• ~'37 .600 .6131
• '5';"? • .6013 '+ .599 '+
.600 2 .5'39 :3 .598
* PRISE! LAT. GAUCHES* 4 .598 5 .5',8
.5,,:3
.6~~
.1502 • ;S~0 • ~.)2 • ~ja4 .O:)~3 .6134 .606 .'::01 .602 .5"1
'+ .5'?1!i * .6.)2 *' .613:3 * .59', *' • ~'J1 ,. • 6~31 ;; .601 '+ .~02 * • 5'?3 ., .601 * .59', ., .l!i1il4 +.
:;.
6 .598 7 .598 :3 .59? " .598
113 .598 11 .599
HLIS. rWAL
.602 2 .602 3 • ~a2 4 • ~a2 5 .601
PRISE! LAT. DROITES* 6 .~al
74 75
· 6.)~ .5'?8 .5'37 .5',', · 5'~8 .5',7 .5'?9 .5'?6 .598 .5'?:3 .5'3:3 .597 · ~.j5 .59:3 ,~6S .'5% 0667 .6131 .61~ .6132 .613 .601 .~14 .602 .611 .6133 .610 .6.)2 .6113 .6131 .614 .5'", • 6~9 .59', • 6~)4 .59:3 .6>33 .600 .6')0 • 6Y)~ .6133 .5,,:3 .598 .6133 .5:39 .61)1
PR X3E'3 COL
.615 .. ; 1.1)64 · ~.~~~ , ,,~::1( • :302 .7"9!5 • :36:3 • ~'~2
1.02:3 .6:32
--
* f .~a2 ;;. :3 .61:34 ;;. " .6134 ;<, 1~ . ';:02 ., 11 .6al
.~
:3 4 5 -
.6135
.6as
.604 ;~01 .601 .60:3 .6VS .~a6 .6137 .-51315 .~a4 .6as .604 .6134 .6.n .601 .6al .-5131 .6131 .6132 .~~2 .60:3 .~01 .604 .604 .6135 .6'.17 .6ae .6013 .604 .6134 .602
MACH '"
• ~01 • · ~el * .~al ;; .~131 ., .6131 '+ .601 -+ .600 ., .601 -+ .601 ;; • ';131 ~ .';13~ ;; .600 '+ .598 *'
HUS. DROIT ;<,
• 5','~ .59', .599 .59:3 .5',:3 • 59'~ .'B" · 59'? .'59', • ~9', .593 .539 .S,9 .59'3 .59:3 .5',8 .53:3 .5',:3 .5',:3 .'599 .'599 .599 • '3,,'~ .5.,9 .5',', .'B'? • 'B:3 .59', .5"'~ • 59'~ · 5'?'~ .599 .5',9 .'599 .599 .599 .5'3:3 .'5',', • SSI:3 .5',:3 .598 .59:3 .5'?:3 .598 .59:3
2 3 4 5 <5
37
"!ACH
.'570 · 5:31 ,';.2:3 • 6:31 • ~;3'J .651 • ~: 11 • 5'~'~ • 3:3iJ • ;::~2 'j'.,'" · '.'.-
• 7';~ ~ . .,.~
• I oJ ...
. 710
.712
.702 • '::'~8 • ";'~:3 • 6'?3 .6':1 • r5;32 • ';:3 ~J .- .... .r, .. ..;.
.5~1
.5:31
.-527
.~~:3 .:~.., · ,~ .. -
.64'?
.62'5 ,,-517 .303 • :3','~ .... ~ . ., • I , _
.740 • 73~) .i24 .7'21 .71 r; • ~~J~ · ';','? .-5'35 .-5?O • r5,3~ ,~67 ,';r5'; • 66~j , ':'4» t ~r3~) .';:2.7
129
"'*************************.*** FICHIER AD139 N0(IT'= 1 22/ a/8~ l1H 0 AS07 M=.a I=0(-30'+ROT.30') R 2-5 NON ADAPTE AD13~ DE AD44~ l'ITE PAROIS RECTILIGNES + 30' -------~ACH-DE-;EFERE~cE:-~8e;;------~I~F:--z;i~io9-~~S---------------------,·
TIV=301.2 K PIV= lS51 MB ~**~~~~**~*~~*~~*~~~~*~ .. ~~~~~*~~~ .. ~~ .. ~~++.~~~*~**+.~~+.*~~~~**~~~~+.~~~~~~~.~~.~"
2 3 4 5 6 ., ,
MACH PAROIS HAUTE ET SASSE MACH PAROIS LATER.
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r',ACH ;+
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• 5'~7 .5';'7' • S'~7 • 5'~7 .5.,7
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21 .,,-? -'-
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34
***********.*****.***.****.*** FICHIER AD145 N0(IT)~ 4 22/ S/8~ 17H15 AS07 Ms.6 !2+2 R 2-' ADAPTE ZD AD14' DE AD131 4' IrE. ---------------------------------------------------------------------------.~~ MACH DE REFERENCE= .5959 urNF. 231.10e M/S
2 :3 4 , 6 7 ,~
"
"
113 11 lZ 13 14 15 16 1;' 1::) 1 " 29 21 12 23 24 25 21'5
TIV=297.1 k PIV~ 1391 Me
MACH PAROIS HAUTE ET BASSE * MACH PAROIS LATER.
HAUT
.5',:3
.5',9
.5',8
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5'=-':' .5',', • 5'~'3' · S',', • 5'?'~ , S'?8 • S';'4 .'591 .5:36
BA:;
.'93
. ,'n • 5',6 .,% • 597 • 5,,8 . 5% .5',5 .5',6 .sn • 5,,4 .594 • 59:3 .5',4 • 5',5 .5"4 • 5"4 • 5,,3 · 5,,2 · 5',4 .593 · 591 .589 .5'H .592 .592 .5"1 .5n .592 .59:3 .58', .592 • 592 .591 .5',9 .592 .5',0 .5',1 .5',1 .591 .5'?1 .5'H .5n .59:3 .592 .592 .592 . 592 .5',:3 • S'?S .5',5 • '5',4 .5'?5 .5',5 .5n .sn .591 .5:3:3
HAUT ~lACH
..; PRISE! DOUBLES • HUB. AMaNT • * S'?
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.. 61
.5'?6
.5'?8
.5',7
,5915 * .'5% • .5',5 '+
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..;. 62
.. 6:3 * 64 ... 65
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10 .594 11 .594
HUB. A"lAL
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..; PRISES LAT. DROITES. 6 .599
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• ·"55';' .6'?S · 7'~6 · '3>5.3
1.~:121
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1. ~j57 • ?~3:3 • ;-'?'3 • ~'31 .631
7 .598 * :3 .59', * " .598 * 113 .597 * 11 .597 * ;t HUB. GAUCHE
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30 .60:3 31 .601 "32 • S':8
MACH ..
:33 • 597 ,~
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TIV=297.e K PIV~ 13?3 Me ~*~~~*~*~~~**~~~**~~~**+.~*~~~**+.+*~*~+~*~~,~~~*~*~***~*~*~ .. *.~~~~~~~~~.~~~~~~~
MACH PAROIS HAUTE ET SASSE MACH PAROIS LATER.
HAUT
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.5'?6
.5St'3
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HAUT r'lACH
PRISE~ DiJUSLES * HUB. AMONT
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PRISE3 LAT. DROITES* 6 • 5,S
74
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* :3 .5',7 ;; ., • S96 ., H) .594 + 11 .5,,3
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.5'?'': * • 5',1 + • 5'? 1 * • S:35 * .~8:3 *
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.~S3 1.g~:~ ~ 14 .5~8
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~ 2'~ • ~.a2 ;; ·310) .05130 +31 .5',', ., 32 • S',5
r'lACH * :33 ,5';4 ~ :34 .5n • 3S .5n '+ 36 .sn '+ .37 .5931-3:3 • 5'~2 * :3', • ~',Z -+ 4~ .591 '+ 41 .5',2 '+ 42 .. 5',3 ..;. 43 • '5'31 '+ 44 .598 + 4'3 .5910) ;;
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:3 "
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• " .. I ~ ... ~
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MACH PAROIS HAUTE ET BASSE it it
EII=t:~ it it
MACH PAPOIS LATER.
HAUT
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• 5'?~ .5:37 • S:34 .5,'::-.5'~
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* PRISES DOUSLES
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• S3', .600 .5;";' · 5,',
* HUB. I~AUCHE
2 :3 4 S 6 7
27'
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t1ACH ,.
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"
10 11 12 13 14 15 16 17 18 1 " 20 21 ;2;; 23 24 25 26 .-:.-,
MACH DE REFERENCE~ .5936 TI ',/::300.6 K
UINF~ 231.108 M~S P I ', ... ~ 1392 NB
NACH PARors HAUTE ET BASSE NACH PAROIS LATER.
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* PRISES DOUBlES
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NASA TECHNICAL MEMORANDUM NASA TM-88442 r ' /..) <7 J /J .1/. /V {; it: -. / 2 "{I' ( -1 i
AO~\PTAT'\O"~ TESTS WITH THREE-DIMENSIONAL ABJtJ5TMEN'l'S IN THE RECTANGULAR
WORKING SECTION OF THE FRENCH T2 WIN~~t~NNEL, WITH A. 'T1Pr: AS 07~ SWEPT -... WING,AMODEL I"'~TAL..L..E'O
A. Blanchard, M. J. Payry, J. F. Breil
Translation of "Essais 'd'adaptation tridimensionnelle' de la veine rectangulaire de la soufflerie T2, en presence d'une maquette d'aile en f1eche du type AS 07," Rapport Technique OA 34/3075 (DERAT 12/5015 DN), O.N.E.R.A., Centre d'Etudes et de Recherches de Toulouse, November 1985, pp. 1-24 (plus figures).
N86-28964· # National Aeronautics and Space Administration. Washington. D.C. TESTS WITH THREE-DIMENSIONAL A[)JUSTMENTS IN THE RECTANGUu\R WORKING SECTION OF THE FRENCH T2 WIND TUNNEll. WITH AN AS 07-TYPE SWEPT-BACK WING
~ MODEL A. Blanchard, M. J. Payry, and J. F. Brei! Jul. 1986 161 P Trans!. into ENGLISH of "Essais d'Adaptation Tridimensionnelle de la Veine Rectangulaire de la Soufflerie T2 en Presence d'une Maquette d'Aile en Fleche du Type AS 07" rept. OA-34/3075, DERAT-12/S015-DN ON ERA, France, Nov. 1985 p 1-24 Transl. by The Corporate Word, Inc., Pittsburgh, Pa. (Contract NASw-4006) (NASA· TM-88442; NAS 1.15:88442; OA-34/3075; DERAT-12/S01S-DN) Avail: NTIS HC A08/MF A01 CSCL 14B
gn text until
The results obtained on the AS 07 wing and the working section walls for three types of configurations are reported. The ....... ..I"C..-"'""-
first, called non-adapted, corresponds to thf~ divergent upper and lower rectilinear walls which compensate for limit layer thickening. It can serve as a basis for complete flow calculations. The second configuration corresponds to wall shapes determined from calculations which tend to minimize interference at the level of the fuselage. Finally, the third configuration, called two-dimensional adaptation, uses the standard method for T2 profile tests. This case was tested to determine the influ~nce of wall shape and error magnitude. These results are not sufficient to validate the three-dimensional adaptation; they must be coordinated with calculations or with unlimited atmosphere tests. Author
to{ ~b NISTRATION 1'{~
JULY 1986 1£ Experimental nr _ Step~ NASA Langley
5 Br~t~ :~~665-5225, USA. Center, Hampton,
l ~~ .. --. --------'-----'
NASA TECHNICAL MEMORANDUM NASA TM-88442
/V 2 10 -, ;;~ 2 C; (I' 1/ 4( AOAPTAT\O,.!>
TESTS WITH THREE-DIMENSIONAL Af)JtJ5TMEN~ IN THE RECTANGULAR WORKING SECTION OF THE FRENCH T2 WIND T~NNEL, WITH Aa
I~"'''' T1P~ AS 07~ SWEPTiAMI!iC WINGAM DEL IrJ£TA'-\"£C
A. Blanchard, M. J. Payry, J. F. Breil
Translation of "Essais 'd'adaptation tridimensionnelle' de la veine rectangulaire de la soufflerie T2, en presence d'une maquette d'aile en fleche du type AS 07," Rapport Technique OA 34/3075 (DERAT 12/5015 DN), O.N.E.R.A., Centre d'Etudes et de Recherches de Toulouse, November 1985, pp. 1-24 (plus figures).
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further notice:
.~
NATIONAL AERONAu'!'J.CS AND SP WASHINGTON, DC 20546
E ADMINISTRATION ~f~6 JULY 1986 If Experimental
E S~~oS1~ ~ASA Langley r. tOP 2, 25 USA
'ques Branch, a1 n VA 23665·,52, ' iechn1 h Center, HamptO ,
p.esearc
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PIi! 6 f' •• I •• "';n~ O.~.n;.c>';c>n Coc!. THE FREf:J~!:k T2 WIND TUNNEL WITH: O'IAS' 07~ SWEPT- ' ~ WIN~"MQDET. 1",~~Ay.....E" 0,
7. A_u.ho,(ol A, '1 Blanchard, M. J. Payry, J. F. Bre~ ~--------------------10. w •• 1. Unit No.
------------------,------i". Con".".' ~ .. n. Hc>. ~. Pc,ll)"n;n~ O'SO"\i •• "on No", • • n~ I..Ji, •••
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13. l,p •• f ",p." .,nl P •• iol Cc>w ... l
Translation
Administration
l~. Supp·',",.n'o,,, 1'10'.1 Translation of "Essais 'd'adaptation tridimensionnelle' de la veine rectangulaire de 1a soufflerie T2, en presence d'une maquette d'aile en fleche du type AS 07," Rapport Technique OA 34/3075 (DJ;:RAT 12/5015 DN), O. N. E. R. A., Centre d' Etudes E!t de Recherches de Toulouse, November 1985, pp, 1-24 (plus figures).
- t.' / £;:{t-~~l 1 tl. A~.ltoc' This report pre ents the resy'l ts obtained on the AS 07 w4-Rg and the • working section walls fo~ three typespf configurations.' The first,~~tt.ed 11~~~ "non-adapted,'!!~~iresponds to ~ divergent upper and lower ~ctili~~Jalls b~)I\
. which compensate for ~~ayer t\\"fc-i.~~H1g •. It can serve as a basis fO'r ~=---, .... \~'A< r- .pletoe .. flow calculations. The second configuration corresponds to wall shap~s
o determined from calculation's which tend to minimize· interference at the level of the fuse;Lage. Finally., the third 9?:nf~~ calle~ "two-dimensional adap.ta-tion! II uses the st~mdard 1!lr.th~d, for~_ ~ests, This case was tested to determine the influence 0 ~waIl'i:ha a ana-error magnitudeS. These ~esults are' not sufficient to valida 'the th e-dimensional adaptation; they must be coor-
dinated :with ca1CU~~iQ s o~ Wij~~J~es.ts. "
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TABI~E OF CONTENTS
NOTATION
1 - INTRODUCTION
2 - ADAPTATION PRINCIPLE 2.1 Two-dimensional adaptation
2.2 'I'hree-dimensional adaptation
3 - EXPERIMENT EQUIPMENT 3.1 Working section equipment
3.2 Mounting the wing ~ 3.3 Acquisition and &XemiRatlonrprogram~
~~~J 4 .. SUMM}~RY OF TESTS MADE
5 - CONTROL TES~ (4 ~ JLw ~ 5.1 ~ by wall rotation
5.2 ~n"\convergence. 5.2.1 Three-dimensional adaptation
5.2.2 Two-dimensional adaptation
5.3 Non /2.0/3.0 comparison
5.4 Visualizations
6 - SYSTEMATIC TESTS
7 - CONCLUSION
REFERENCES
LIST OF FIGURES
ANNEX 1 - Cz
2 - Kp
3 File listing
Rages
4
5
7
8
8
9
9
10
11
13
17 17
17
17
18
18
20
21
22
24
25
tI
3
~~~--~~-------------.------------
NOTATION
~:) Cartesian coordinates in the reference working section zp (porthole axis)
: X} Cartesian coordinates in the wing reference (leading
edge to socket)
C Profile chord of the wing section considered
Angle of the model (fuselage axis)
-r;J; ~ Mo -I-nfiliiLe Mach~~t~~=tIt--=the· 'l:~
M Local Mach (wing or wall)
Kp • p_po
! p Vo2
2 J. Pressure coefficient
Cz Local or complete-wing lift coefficient ;
= ( Kp. d(cb) J.".!iL
tI
J 0 vI Vi-I)
Ao ~P~,..IC:>"'.s TESTS WITH THREE-DIMENSIONAL ADJUS'PUEN'rS IN THE RECTANGULAR
WORKING SECTION OF THE FRENCH T2 WIND TUNNEL, WITH·Am T-tPr: AS 07~ SWEPT 'BACK WING MODEL 1",~r"'I..\..ED.
A. Blanchard, M. J. Payry, J. F. Breil
1 .. INTRODUCTION
This test series follows a study done in the T2 wind tunnel ..
with the goal of defining a shape for the adaptable walls which
would minimize their influ~ on three-.dimensional objects ~ placed in the center of the~section or fastened on the side~~.
-to k . ..,.et I,'(\~h r".J,,~. -'>--:tll (1 I
The presen~onf~u~a7!f~t~ working section does not:rL~·{V)"O:VICI. allow ob~§ .. shape~ iderrtical to that of the layGC Of~. ~ -.A...:...i... • +-~ d th d . . 1 d 1 . .. . t· 0 GY-r~ eX1S~ aroun a ree~ ~s10na mo e 1n \Hillmlted- ~""~
atmosph~~ (two completely rectllln&ar and parallel lateral . ~ walls, two flexible and bendable upper and lower walls). The
planned solution thus consists of using the two bendable walls to minimize the influence of the walls on the model.
The method implemented uses solutions developed by "E.
Wedemeyer and L. Lamarche~r~A first series of tests was
done in cooperation with the~University of Berlin on various
existing models [6]:
- a CS revolv.ing body 166 mm long, 0.3% blockage;
- a civil F4 airplane model with l20-mm wingspan and three-
component balance;
- a duck-type military airplane model with the same balance.
Another series of tests was then done on a bigger model £7]:
- a CS body 400 rnm long, 1.8% blockage. tI
*Numbers in the margin indicate pagination in the foreign text.
5
The rE!sul ts and calculations were compared.
The calculation methq9 was optimized for re'~l!tin9 bodies ~ ~ \.c.~~; j-placed in the center of the~section, an extrapolation was tried which placed a half-wing at the wall. In this case, calculati()n~ -i-s- done as if the section were twice its actual width, using the
Mach distribution at the wall measured near the plane of
symmetry.
The results obtained on the "16/1000-scale" AS 07 are
discussed in this report. They can be divided into two groups:
control tests and systematic tests. fL" :;tt. Included in the first group is control of wing anglil~ by
rotating t:he walls. The ~ of the jacks would not permi~e~;J1.1 tJ displacements ~<Lhr calculat~ for ang'; fig eft@ model Q" 'I
cI \\
+2-, we thus used this artificial method after AaviRg verif~~~
its validity.
The three-dimensional adaptation method supplies the WI"\
optimCiiA: shape of the walls from the first calculation, whatevEH the initial position of the walls, this was verified in /8
several test configurations. Finally, an adaptation called 2-D
"~dimensional" was tested; it uses the normal method for ~ 2.0
prefiW-t.ests. This case, without theoretical justification, . ~ "-....,CoI,)
w~fdied "'£'0 ~h:r~blPee~ceof the sa ape ef the wall,),.and the ~.e eftrro~~
The second part of this study corresponds to systematic tests: four configurations were chosen w~ich gave different lift coefficients, without making highly supersonic zones appear on the profiles. For each configuration, three wall positions welre tested:
- The first, called "unadapted," corresponds to the upper and lower divergent ~eeilift8a€ walls compensating for
6
\ .. ''''.''C~ "'"I ~,.
~1)l~~'--~r bO'~
thickening of the 14~ layers; it served as our basis
for beginning three-dimensional adaptation calculations. These particularly simple limit conditions can also be
used for complete calculation of the flow in the working
section.
- The second adaptation
positioned
wall shape comes. from the t~-dimensional
calculationJ the flexible sheets are before the ~_~ ~ ~,
~1'--
- Finally, the last case corresponds to "two-di~ensional .
adaptation"; the iterative process converges ~ a single
C}U+t.. b.-l "'-. /j,{L";-"v'·
~~ For each type of test, three 9tl8t~are necessary to obtain
readings from the six rows of pressure recorders spread along
the AS 07 wing.
The experimental results gathered during this series are not sufficient to validate the three-dimensional adaptation
method used. Additional calculations ~st be made to estimate residual corrections. In these tests,' Ii "- n~eJ::;l influence of
the walls is observed for low lift values or low Mach number
inversely, for 2 degrees of incidence or for Mach 0.8, the iSiI~~~II~~ become significant and can in part be interpreted as variations
in aerodynamic incidence.
2 - ADAP'I'ATION PRINCIPLE
._~_E-~~o purpose of the adaptable walls is to create an ~~~flow around a model, in a working section with finite
dimensionsJ this can be done by controlling the wall conditions, either by their shape in the case of solid walls or by flows of
mass through porous walls. The first solution has been chosen
at T2,~e flexible sheets moved by jacks form the upper and
lower ~of the working section [3).
7
~---~-___ -"-------·------------_.L In the case of a three-dimensional body, it is necessary to
bend ~ w.111s. lo;.a~ed a~.':'~\;-~';...-\,m~ob~el to arrive at a shape ~ ~ Ml':r I;;'f zhr1-~eXiSting around the model in\»I'I~Uoed4
~~~~~~~e~E~ This solution is not at present possible .£ T2, but
on the other hand it is possible to use the two flexible /9
/. j . ' '.~
walls to minimize residual corrections due to the influence of
the walls on the object~.
2.1 Two-dimensional adaptation
The details of the process will be found in [2] and
(4); it uses a coupling between the real ~16w in the working l~,,:,\''''''''!.~
section (internal field) and a calculated vir~ua~flow outside
the wind tunnel (external field). Coupling occurs on a control
surface near the walls through speed vector components.
Adaptation is achieved by an iterative ~:~a~ing on the shape of the walls: the components of ~a ~ the control
surfac~come,available at each iteration; they are
extrapolated from the pressure measurements at the wall. The velocities needed on the control surface to achieve an unlimited
external flow are calculated by the Green function following an inverse method. A method of optimized relaxation·between the
internal and external flows for the vertical velocity component,
followed by an integration along each fleJcible wall, supplies
the !!'lew shape of the wall. The real shape needed is obtained by
adding the thic;kness displacement of the four wall limit layers.
2.2 ~hree-dimensional adaptation
For three-dimension~tion, .the process is different [5J: it uses ~ of the model through b~ ~ distr ibution of sourc~ vortices i~W hor~eshoe)
Plac~th~ection ~i This s~atiaat10n ~iv:& a good ;;Urea.entat~~of ,axisymmet :ical bodies mounted in the middle of the working section.
- ) 13 r, ('J,~\' ;.'1 -t/l"l
8
The originality of the method lies in then doing a
linear trclnsformation, which permits passing directly from distribution of velocities at the walls to the adapted form without needing to determine the intensity of singularities. The optimized shape of the walls is thus theoretically obtained from the first calculation; this shape, which is not exactly
"adapted," minimizes residual corrections on the model caused by
the influence of the walls.
1: Using this met;hod ~f-wing at the wall.is "!J';'! ~, because the ~m ~iliati;;t·does not r~~t""2.a wingspan~~~~s nonetheless been tried here by replacing ehe ~
lateral ~~ by a plane of symmetry leading -to a fieti6"al~~ double section width, and t.aking the Mach distribution of the ;Jr..i..:/;'.
c'IDl{<l..-'
flexible walls near the plane of symmetry as reference.
3 - EXPERIMENTAL EQUIPMENT
u- be. J. The T2 transonic wind tunnel is pressuriz~ and can
function at low temperaturE~s; only minimum-pressure and ambient
temperature tests wer~!:Q~during this series.
3.1 Working section ~uipment
The working section has an almost square section of 0.39 x 0 .. 31 ~2 at the entrance. Flexible sheets of Invar
make up the upper and lower walls, equipped with three rows of
pressure recorders whose coordinates are given in figures 1 and
8. The s~llt-pOSi tioning mechanism is descr ibed in [2], [3],
and [4]. <gt!;~delV}A I
:i:ixi
The left lateral ~ has three portholes with pressure recorders placed along horizontal and vertical lines whose coordinates are shown in Figures 7 and 9.
9
The pressure rec()rders are linked to bite Scanivalves,
each Of~~~ can obsE~rve 48 positions in 5 seconds.
The position of the wing in the working section is
given in figure 6. 1~~'o(1t;
;~C~ The Mach number ()f the flow is set by a seeef'ld -~ controllE~d by the computer which controls the ~. ~ ~ .
No other equipment or wind tunnel measurement meth()d ~
we-s used ..
3.2 Mounting the wing
k..t~-The AS 07 wing.\model with a scale of "16/1000" is
shown by the photographs in figure 5. The method of mountin~J the wing on the wall is shown (figure 6), the plane of the wing
and its specifications I\~fe y.iven .(fi~~a~, and the shape of the profilet:~~ it.,and the positions of the pressure recorders are indicated (figures 12 and 13).
cd- cG'1 tW ",Y ~~vLV ,"-.lC h-c.<>U"." M.9. ,1.. ~'Y')
There are six rows, each with 16 recor~ers on the inner and outer sections and one on the leading edge; they are
placed across the wingspan so as to form lines with constant chord percentages. These recorders communicate with tubes placed in grooves along the wingspan; each tube communicates
with three recorders (either on the external wing or on the internal wing). When one of the three rows of recorders is used
to measure pressure, the other two are covered with thin (0.05-mm) adhesive strips. It is thus possible to simultaneously measure pressure on two sections of the wing (one internal and one external); measurement of velocities over the entire wing thus requires three different gysts.~ ~~
porthole, The wing is mounted on a half-fuselage linked to a n rotat~ 4:8L;~aR91iA9 ~ll~g-
/t"tat't.4 ~+~ i.-/ 10
fuselage assembly; on the back of the
the angular reference is the r~~a. part
fuselage [1).
3.3 Acquisition an'2~l2rOgram. The T2 wind tunnel is linked to a _t~_~-D~f,_two W =
computers, one concerned wi.th creating and ~ the g.y.s..t
and the other with obta~g_data and storing measurements to
disk at the end of w.e ~~ ~. ~
These tests are Purs~antLto the series done on the /11
C5 body and use its principal elements.
Disk cart:ridge LU 26, Program LU 34, Test files, calculation files
Acquisition program
(TEACQ)
(RAFAL)L PARC 5
or
PARC S
(lance ACQC5)
(uses PROJ and ADAP.)
Fixed walls:
No adaptati~n ~
during ~:~ ~
Two-dimensional . adaptation
Ini tialization of programs {With (TR,) RINC 5 (For PARC 5)
or (TR,) RINC S (For PARC S)
Test file
AD ,--- test number from AD 100 to AD 173
11
II
wall positioning 'file -- any test file - or calculation file _ or"special file AD 4:
AD 444:
AD 445:
AD---
AD 9 ---Divergent t:e;~a~ walls;
symmetrical ~ayers. ~
AD 4 + 10'~rotation upward 04(.~ •
AD 4 + 30' ~rotatlon upward
Three-dimensional adaptation calculation
Calculation from a test file AD ---
VKJ 43 Calculation of wall shapes without rotation
VKI M Calculation of wall shapes with rotation
! LJ)
I ?l:::=---
.... --- - ---- - - - --. 780 "''''
---tFiling to disk I
.. I I
: ~& 310 mlft
. ,
!1le for new calculated wall shapes
- section length 780 mm
- ratio c = hlb = 2.1081
- reference recorders:
right lateral RL
- weighting coefficients
file VKJ - R (cartridge
LU 43)
AD 9 --- beginning test number for the calculation
E!0gram~; for examination ()f AD--- files
L'l'CS:
- graphs local profile Mach numbers
- graphs Kp - lists AD file
- calculates Cz 12
LTC 51: - graphs wall Mach numbers - graphs wall shapes
starts LTC 52 (does eln RP, LTC 52)
LTC VK: - graphs only wall shapes calculated by VKI 43 or VKIM
( from AD 9 - - -) •.
- SUMMARY OF TESTS PERFORMED
A previous study was done on the AS 07 wing (1]. We
erified in one case that the same results would occur, althou9h~ o. (j he working section was modified when the T2 wind tunnel was ~
fOlr cryogenics.
The first control tests were done by measuring rows 2 and 5 pressure recorders for the Mach numbers and incidences
cHeated below:
-~ 0,7 0.8 )
) - )
+2° X X X )
0 X X X ) _2° X X )
-)
13
Four configurations were selected for systematic tests: L!l
-)
0,6 0.7 0,8) )
(----=*--~---:---:) (+2° X: : ) ( ::) --- ------- ---- ---) ( :: (0° X: : X )
(------- -------:-------:-------» ( . :: (-2° X ) ( )
'ltL.u') ~ v6.{JL4-)
hey correspond to a sampling of lift coefficients and ~ ofi~e Mach e£fe~£ee~, while limiting the supersonic ones which appear on the profiles.
Figure 1 shows the list of tests in chronological order,
nd figures 2, 3, and 4 classify them by configuration.
We first Sho~:.~~r~~:ijln~~e uppe~_~I!.i ~ower walls as equivalent tO~Athe m;Jel at 1[he sam~~. This~~O.--.--~ ~~ was made necessary because the ~of the jacks did VV~
-&,-o.""uv . t permit the displacements required by calculation of
ree-dimensional adaptation for a model incidence of +2".
- DivE~rgent ~QtiliRQa~ walls I
·Mo ( )
0( , ( 0( " •• 1.1 0,6 0,8 ) 6tllotd .• ( 0\$ a.: ·-s.tw l
( )
+2° ( +2° AD4 AD 120 : . ) ( +1,5° AD 445 AD 122 ) ( ----- _.- ------) ( )
O· ( 0° AD4 AD 107 - AD 109 AD 108 - AD 132 ) ( -0,5 0 AD 445 AD 137 AD 139 ) ( )
14
- !!!!.ee-dimensional ada.E..ted walls
Mo
( ) (0( CALCUL 0.6 0.8 )
Q( afrod. • O· ) )
(:---, ( ( O· VKI 43 117 AD 119 ) ( -0.5- VKI M 138 AD 141 )
(,------------~~-----.~-----------)
The three-dimensional adaptation method theoretically
supplies the opti~ shape of the walls from the first
calculati(m~~atever the initial position of the flexible
~. C~ls were done in this respect for the following
configurations:
Mo ( )' ( 0(, 0.7 0.8) ( ~~pl .. " ) ( ) ( +1.5· AD 127 (I) ) ( AD 128 (2) ) ( : AD 129 (3) ) (------ -------:--------) ( :) ( 0° AD 115 (l) : AD 118 (I) ) ( AD 116 (2) AD J 19 (2) ')
( -- -------: ----) ( ) ( -0.5· Al) 140 (I) ) ( Al) 141 (2) ) ( : ' )
e figure in parentheses after the file number indicates the rder of the iterationJ the wall-positioning file thus results
calculation of the preceding test. (Iteration (0) is the
est don~! with Jr~f~~~e5.walls.)
We also verified that the tests called "two-dimensional aptation" converged rapidly, as is the case for the prcfile 2D
ests; it is sufficient 1&F-:::tOQ:a:t to compare the wall position~ of
15
---..... ----......... ~-------.. -
the 3rd the same ~; the two
positions are always close. In general, the beginning shape chosen is near the adapted shape, but we have tested this
convergence in the two particular cases when the beginning shape
was far from the adapted shape. cl ~ b~'i.. f~ Ch!_e~s \ .... L.A
AD 4: ~~f!.iw.:rwalls diVerge~~'·d·' __ J.;;-s,~ptf, .. :9v ~. C.J-tk.;
~ Lt m~. " M-J~1'\A-y,jj;UL-CrJJI.~,,: t L -C <> ud". ~ /15
Configuration: Mo = 0.7 ~ = +1.5-
Configuration: Mo = 0.8 « = o· File AD 130 (1)
File AD 133 (1) followed by File AD 134 (2)
Comparisons were made between the various wall positions;
hey are noted:
sb~l4 - "Non," for divergent J~ctlliftear walls
- "2D," for two-dimensional adaptation done with the PARes program
- "3d," for positioning of the walls in the shape
calculated by the VKI 43 or VKI M program
It was decided to do systematic tests for the three cases
f "adaptation," the non-adapted case serving as a basis for
hree-dimensio~al calculation (any wall shape will work), this
ase can also ~erve as a basis for complete flow calculations,
ecause her.e the limit conditif~e particularly simple. The
wo··dimensional adaptation, ~;;;S~ the subject of the
tudy, was systematically tested to use as a comparison with the """"" ssumed optimai shape.
Finally, four configurations for three cases of adaptation,
~produced three times to h~~~ocity field on all of the lng, were tested; these 36 ~~make up the systematic tests isted in figure 26a.
16
5 - CONTROL TESTS
We will not present all the tests done, but only a selection of cases judged most interesting, since the goal of
this series ~not to evaluate the AS 07 wing. /' L_ _ 0 ,0 A () (' h \ n" ~. ,D i' , ) rn . '7 r" ~r~,-. ~~. CA/I (( t I('~'L ~ "'''(c, __
5.1 Arflg1in9 by wall rotation '
, ~ Of the five configurations tested (para9raph 4), three
are presented. The first corresponds to Mo = 0.6 and ~ = +2"
for ~trl~~.r walls (figure 14); this is the configuration
which obliged us to use this~e:, as the three-dimensional
case could not be tested.
Figure 15 shows the comparison of Mach numbers on the
walls and on the wing, for an aerodynamic incidence equal to O' and a Mach number equal to 0.8, in the case of £eetiliRear6f~~ walls. Figure 16 presents the same configurations but for wall
'¢D . shapes c:oming respectively from~calculatlons VKI 43 and VKI M.
;S :J) aaLl P :1:: o---~'/
The results of figures 14 and 15 sho~hat the high ~~~:~~ ~ ----. Mach case is the most , but the.!Cor=. dence'-of the
tests remains good. Figure 16 ,shows that the VKI M calculation o...c....o
makes perfect allowance for ~otal rotation. ,
i ~~. It· is thus possible to display a model incidence ill
different from that desired and to compensate by rotating the walls.
5.2.1 Three-dimensional adaptation
~veral calculations for optimization of wall Shape wereJ;oRReetedlfor one configuration. The last test is
always recalculated, leading to a wall shape which by definition
17
ill not be used, but which will in fact constitute an
dditional iteration.
Of the four tested cases, two are presented in
igures 17 and 18, the first (Mo = 0.7 and = 0·) shows that he adapted shape is practically obtained from the first
'terationJ in the second case--much more difficult (Mo= 0.8
nd 0(= +2")--it is necessary to wait for the second. Q ~ -11> alculation. This second case corresponds to a freely ~ U ~6 upersonic regime of the wing which will not be studied
ystematically herein.
5.2.2 Two-dimensional adaptation
In all tests done, the 3rd i ter~~ J! always dentical to the 4th and last iteration of the ~, even when
he upper and lower walls have been prepositioned in a shape ery different from the "adapted" shape. This is the case shown
n figure 19 corresponding to Mo = 0.8 and «= 0·.
To confirm the validity of this statement, a
econd test was done, positioning the flexible ~~ on the~ receping shap~ the values obtained can thus be considered to
orrespond to the 4th, 5th, 6th, and 7th iterations of the test;
hey are all identical (figure 20), which confirms that the
onvergence was lwell obtained.
5.3 ~)n/2-D/3-D comparison
Two cases are presented here, one Qf which is not part f the systematic tests:
Mo = 0.7 - Mo I: 0.8
(){ = 0"
18
The bervea following tt~es of "adaptation"
become more significant as lift aR~~Mach number ~pstt6am increase. The adaptation called "two-iiirnensional" gives results
nearer to the non-adapted case; in fact. everything happens as if the aerodynamic incidence of the two~oimensional case were
igher than that of the tests with~a wt!l shape adapted in three imensions. On the other hand,rre~tIti~e-aFLwalls lead to a
igher effective Mach number upstream ~'blockage effect).
In the first Ca~ffigUre 2U" the ~e moderab~; hey are more significant~n the seconO! case (figure 2~ bservation of the 8~ti~2of the walls leaving the GOAver9~t figure 21) shows that,effectively) the direction of the flow
pstream is no longer horizontal in the "2-D" case, unlike thE~
3-D" case; the angular referen<?e.91as j,i.ven by the "non-adaptE~d" The effect produced is i-neon~e~'a\le7 because we /17
reviously demonstrated that rotation 0,£ the wall~Q!5embly
odified the aerodynamic incidence of the model; ~owever, this
s not sufficient to prove thal, the 2-D case is &~=s, ~~ ecause the direction of the etJ.~~~t~ lines inll"liliittea.~...J. -
~ .£.ti,: UVYt~-., v--'>\ C-t> ;"''\A~ 12 • ... ~~:.w.t~e-T·'5.~not known. We note also the very different shapes 0-'1.1.)
f the walls downstream; they go downward for the n3-0 n cases f
hich is logical allowing for the chosen ~jzat~ ~ orseshoe vortex) and the calculation made (in the plane of
But on~e more, that does not prove that the shape btained is optimum.
r (
Finally, one can observe on the last figure (23) that
e effectJ~liElea b?,Zmodifying the shape of the walls is not:
nstant across the wingspan. This was predictable due to the
rking section geometry itself, allowing for twist of the wing
d for three-dimensional effects.
19
G
tI
5.4 Visualizations ff()-t-v..J
For thr~e configurations, oil~sualizations were done 6~~~f h ' , " h d' on the left 0 t e worklng sectlon, glvlng t e lrection of
~~c:.""'~2. ' 4 f' h d f h ' the e~££e~ llnes 55. mm :rom teen 0 t e wlng. Reference marks were made, making it possible to locate the positions
St ... t."'~ "'2 ' , ." relative to the eurre llr~es and to measure thelr devlatlons.
- Zoo -- . --+. _. --..-. - . .-...... - -.- ._f-.-YI"tUt..,'1~ '!.e(..{ ... C')
fl. .... ..
... ",
The end of the wing is located between the abscissas 91.06 mm and 135.86 mm from the porthole (figure 6) and very
near to the section axis (function of the incidence).
The maximum deviations noticed are located on the~ section axis slightly behind the tip of the wing (figures 24,
25, and 26).1
( Walls dmax ) ( MQ 0( ) ( )
( · ) "Non-adapted": - Figure 24 ( 0,6 +2· "
(5· •••••• 6·) ) ( AD 4 )
(-- ----) ( ) ( 0,6 +2· · (5· •••••• 6·) ) ( 'Adapted 2-D: ) Figlllre 25 · . ( : --) ( -· ) · (
0,6 -2· "Non-adapted": «la,s· ) Figure 26 ( ) ( AD 4 )
20
tI
The photos taken from behind clearly show the L!!! eviations of the ;~;~8A~lines.
_ SYSTEMATIC TESTS
.w~ {or the 36 g.usts,\that lmade up the systematic tests
~t~9';~ 4 and figure 26a), the following information is iven: wall shape (~igures 27 and 28), Mach numbers 6~ the
hree rows of recorders on the adaptable walls lfig~res 29, 30, .s,~ ,
1, and 32), Mach numbers of the left lateral ~ (flgures 33,
4, 35, and 36) following the horizontal axis or the three erticals, and finally spread of Kp on the AS 07 wing (figures
7 to 44).
Numerical values for these curves are given in the attached
est listings. File numbers corresponding in chronological
rder to the experiments were kept in the interests of clarity.
Here will be found a systematic comparison' of the three
of adaptation--"Non/2-D/3-0"--and their influence on the .~~ , t 'b t' ~ , , I h ' t~~ , lS rl u 10nS,WHose pr1nclpa c aracterlS ibs~were seen 1n
5.3.
Finally, .integration of Kp for each section supplies local , coefficiJnt Cz. The values are tabulated in figure 45, were traced along the wingspan of the various
nfigurations tested (figures 46 and 47). It is observed that
e internal wing changes less rapidly than the external wing
ith incidence (figure 46) O~Ch number Upstream (figure 47).
On the other hand, the~tween the ·non-adapted· and adapted 3-D" cases increases with the lift.
21
"
Local Cz)were multiplied by the chord of the profile in the
ection considered; the product Cz • C represents local /19
ontribution to wing lift. The values obtained were traced in his representation (figures 48 and 49); this weighting modifies he appearance of the curves ("elliptic" distribution plane),
ut the observed tendencies are the same.
Finally, integration of the curves in this last
epresentati~n supplies the overall lift coefficient of the
ing, which m reported as a function of incidence (figure
0). We have also re~he lift measllred during the S~c-o..>..o.,I-t
reeed ing ser ies [1], between reetllrn9ar walls for a Mach umber upstream of 0.47. The effect of compressibility is felt
ore as supersonic zones develop on the wing.
- CONCLUSION
~ This series of tests on the AS 07 wing is ~ as a
tudy on three-dimensional adaptation of the T2 wind tunnel. It ses the two flexible walls to minimize residual corrections in
he presence of a three-dimE!nsional model. ~It implements the l'-e~e~C:>'I,.-h..-bo""2
• Wedemeyer and L. Lamarche" method where 9mati2atie~ of he model by a distribution of singularities adequately
epresents an aXiSymmetrical~. Extr~~~~ these
thods in the ;case of a half-~~e~~has no ultimate all it serve~ merely as a preliminary phase, to observe the fluence of wall shape tn various sections of the wing, to
udy the convergence of the method, and to make adjustments
otation of walls, incidence, etc.).
On the other hand, these experiments can serve as a basis r calculating potential three-dimensional flow around the
del. Then, a three-dimensional ebjeot placed in th~ection ~
22
tI
ould be more it would lead to
evelopment, as for axisymmE!trical bodies, of a method of
daptation minimizing the influence of the walls on the model.
At present, it is difficult to know if the shape called Q ~ Ie ~ adapted 3-D" is nearer to the values of unlimited atm9sphere~~ han the shape "adapted 2-Dv" but it is definitely not the ptimum shape. /f,,'V/I\ ... flC)U
I ,
~ Jt J6~( tests will ~~ ~ direc~al ~t).layer
"_e-a4:1+f~2cm the lateral k'lall at the level o,f the ~ the
ingtr. The! direction of the c:lA-~~~'f2Iines in this area will bE! n important element in the E'.eality-calculation comparison~
23
R1~FERENCES
A. Mignosi, A. Seraudie. "Etude d'une maquette d'aile en fleche a la soufflerie T2 de l'ONERA-CERT [Study of a swept-back wing model in the ONERA-CERT's T2 wind tunnel]." DERAT technical note No. 13/5006 DN, March 1977.
J. P. Archambaud, J. P. Cheva11ier. "Utilisation de parois adaptables pour le~tsjajs en F~~~~nt plan [Use of adapt.&.~·~ walls for tests in p.Ta~~lfii"Mrr:- ONERA TP No. 1982-38, AC;:p\I't> ,P-"33S-
}~ AGARD/FOP meeting in London, May 19-20, 1982.
J. p~~~c~ambaud, A. Seraudie •. "Etudes de parois adaptables a T2 ~AClapt:ab1e wall ~~ T2) ." ONERA TP NO. 1983-150, 20th AAAF Colloquium, Toulouse, November 8-10, 1983.
J. P. Cheva11ier, A. Mignosi, J. P. Archambaud, A. " ) Seraudie. "Adaptable walls il:1_~ T2 \.~ind tunnelAQ*'IPT',vG; WA~- ~!>I~ Pril:1~plec, execution, and som~E»Ea~ ~ of two dimensieA&l r~urts.n La Recherche Aerospatiale, 1983-4, ~p. 217=21£.
L. Lamarche, E. Wedemeyer. "Minimization of wall interference for three-dimensional models with two-dimensional wall adaptation." V.K.I. Technical note 149, Rhode Saint Genese, Belgium, March 1984.
6. J. Po Archambaud, J. B. Dor, A. Mignosi, L. Lamarche. Premiers essais d'adaptation des parois auto-adaptables bidemsionnelles de la s£u flerie T2 au~our ~'QQsta~le§.l~ tr idimensionnels [~: · I \. ;atd 0 t test'~ of;t~menslional self-adapting walts ~ ~h~ ~wind tunnel around threedimensional e~~cies]~ ~~A Technical Report "No. 33/3075
, September 1985.
7. J. P. Archambaud, J. B .. Dor, M. J. Payry. Rapport sur la deuxieme campagne du CS [Report on the second C5 series]. (To be pu!blished soon.)
24
tI
LIs~r OF FIGURES
1. Test tables u -
- List of tests - Rows of recorders 1-4 - RowS of recorders 2-5
Rows of recorders 3-6
1 2 3 4
2. ~ount~ng the wing in the section
- Presentation of mounting 5 - Drawing of wing mounting 6 - Drawing of pressure recorders on walls 7 - Pressure recorder specifications - flexible walls 8 - Pressure recorder specifications - lateral portholes 9 - Plane of the wing 10
Dimensions of the wing 11 - Profiles 12
Specifications of wing pressure recorders 13
Control tests
3.1 Rotation
- First control (el = +2·, Mo Wall shape Wall Mach No }1lO-C--Q\ f'\..O
Prof ile Mach 'I'lc>
- Second control (0(. = 0·, Mo Wall shape Wall. Mach ""0
Prof ile Mach ~
= 0.6 Non-adaPt~)
= 0.8 Non-adaPt~)
- Third control (0(= 0·, Mo = 0.8 3-D) Wall sha~e Wall Mach ~ Profile Mach '"'0
3.~A~ergence ~~s A _:;,,;;,.:.:.:..;::.::..;_;z..::.::..:..=.=--==~-==..:
a - 3'-D
- First case (cx= 0·, Mo = 0.7) Wall shape Prof i le Mach N:>.
- Second case (ol= +2·, Mo = 0.8) Wall shape Prof ile Mach "'0
14
15
16
17
18
25
b - 2··D (0(. =0·, Mo = 0.8)
_ Beginning of AD 4 (File AD 133) wall shape Profile Mach -
_ Beginning of a similar shape: AD 133 (File AD 134) Wall shape
19
Profile Mach ~ 20
3.3 ~on/2-D/3-D compari~
( 0<. ::: o· , Mo = 0.7) Wall shape Wall Mach ~
(0< ::: O· , Mo = 0.7) Profile Mach t..(2) Profile Mach~~3)
(0(. == 0·, Mo = 0.8) Wall shape Wall Machn..o
(0< == O· , Mo = 0.8) Profile Machllo(2) Profile Mach 1\0 ( 3)
- (ex == O· , Mo = 0.8) Kp
Visualization, left lateral ~ ~\Qt..J1. - «()I. =: +2· , Mo = 0.6) Non - front
Visu (2) - back
- (ex :: +2· , Mo = 0.6) 2-D - front Visu ( 1) - back
- (C< :: +2·, Mo = 0.6) Ncm - front Visu (3) - back
Use in 4 base cases j
5.1 Wall ~haEe -c..l = -2· Mo = 0.6 -0' = +2· Mo = 0.6
-c:( = O· Mo = 0.6 -0( = O· Mo = 0.8
5.2 ~daEtable wall Mach ~o
- (0<.,:: -2· Mo = 0.6) - Non - 2-D
3-D
'YflctC)\ 'n,(J( 21
21
22
22
23
24
25
26
27
28
29
26
(~ ~: o· Mo = 0.6) - Non - - 2-D - 3-D 30
- (0(. :: +2· Mo = 0.6) - Non - 2-D - 3-D 31
- ("" :::: o· Mo = 0.8) - Non - 2-D
S;~f. - 3-D 32
5.3 I.atera1 },wa11 Mach~ - . - (~ :: -2· Mo = 0.6) - Non
- 2-D - 3-D 33
- (ot :: o· Mo = 0.6) - Non .. 2-D •. 3-D 34
- (0( := +2· Mo = 0.6) .. Non .. 2-D .. 3-D .35
- (0{= o· Mo = 0.8) .. Non .. 2-D .. 3-D 36
5.4 !£ J - (of. = -2" Mo = 0.6) Non adaptahl.e 37
- (0( = -2· Mo = 0.6) - Non - 2-D - 3-D J
38
- (0( = O· .. Mo = 0.6) Non adapt~ 39 I
- (0( = O· Mo = 0.6) - Non - 2-D - 3-D
~ 40
- (-.\ = +2· Mo = 0.6) Non adapt~ 41
- (~= +2· Mo = 0.6) - Non - 2-D - 3-D
~ 42
- (0(.= O· Mo = 0.8) Non adaptabTe 43 tI
27
5.5
- Cz - Cz - Cz - Cz - Cz - Cz
Cz .-
Mo = 0.8) .. Non 2-D
.• 3-D
rreeap ittll.ti :e ~"'M""''''I'-~ Mo = 0.6 (3 1nc.) oC = o· (2 Mac hI f\.o.;Y -ru-V
X chord Mo = 0.6 (3 inc.) X chord 0<. = O· (2 Machl~) (oe.)
44
45 46 47 48 49 50
28
tI
TO :
VIA :
FROM:
D
Dr. Robert A. Kilgore TAD-ETB, M$-287
LaRC/Kaye Lee
NASA HEADQUARTERS NIT~4/ Tim Rowe
r--i '--_. "
Jut 111986' DATE
<jJZl{42.
Per yO_lJr request, the technical translation NASA TM-13~ has been prepared and '-a copy is at1:ached. Please complete the 'blocks and ,~, return this form, after you have read the translation_ If errors are noted, returnoa copy of the translation with your corrections. Your assistance will be appreciated.
A copy of NASA TM- is attached for your information. If you wish f you may completE~ -the blocks below and return this form. Your coop~ration will be appreciated.
TO: : NASA HEADQUARTERS DATE
F'ROM:
scientific & Technical Information Branch Code NIT-4 Washington, DC 20546
NASA TM-
NASw- 4005
A. The Translation
~ o o
Furnished valuable new data or a new approach to research.
Substantiated information available from other sources.
FurfiShed interesting background information.
Other:
3. The Translation Text
c.
o Is / IT Is
technically accurate. _.
satisfactory·v. except for minor deviations.
o Is unsatisfa~t6ry because:
Notes or suggest;ions·: See. ~~ ~
D. Review Campletec:
Tim Rowe
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