effectofwingmodi00lang
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NATIONAL ADVISORY COMMITTEE FOR AERONAUTICS
WARTIME REPORTORIGINALLY ISSUED
September 19^5 as
Advance Confidential Eeport L5G23
EFFECT OF WING MODIFICATIONS ON THE LONGITUDINAL STABILITY
OF A TAILLESS ALL-WING AIEPLANE MODEL
By Charles L. Seacord, Jr. and Herman 0. Ankenbruck
Langley Memorial Aeronautical Laboratory
Langley Field, Va.
NACAWASHINGTON
NACA WARTIME REPORTS are reprints of papers originally issued to provide rapid distribution of
advance research results to an authorized group requiringthem
for the war effort. They were pre-
viously held under a security status but are now unclassified. Some of these reports were not tech-
nically edited. All have been reproduced without change in order to expedite general distribution.
^ CUMENTSOEPAP
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3^ / £ it*
NACA ACR No. L5G23 CONFIDENTIAL
NATIONAL ADVISORY COMMITTEE FOR AERONAUTICS
ADVANCE CONFIDENTIAL REPORT
EFFECT OF WING MODIFICATIONS ON THE LONGITUDINAL STABILITY
OF A TAILLESS ALL-WING AIRPLANE MODEL
By Charles L. Seacord, Jr. and Herman 0. Ankenbruck
SUMMARY
An investigation of the pcwer-off longitudinal sta-
bility characteristics of a tailless all-wing airplanemodel with various wing modifications has been made in
the Langley free-flight tunnel. ' Force and tuft testswere made on the model in the original condition, withthe wing tips rotated for washout, with rectangular and
swept-forward tips, and with various slat arrangements.Flight tests were made with the original wing and withthe original wing equipped with the most promising modi-fications .
The results indicated that changes in tip plan formor rotation of the wing tips did not appreciably reducethe instability at high lift coefficients. Addition ofwing slats, however, improved the longitudinal stabilityat the stall when the slat extended far enough inboard to
cover the area that tended to stall first.
INTRODUCTION
Sweepback is often incorporated in the design of
tailless airplanes in order that high- lift flaps may be
used on the center sections of the wing to increase the
over-all maximum trim lift coefficient of the airplane.(See reference 1.) Quite often, however, the sweepbackdefeats its own purpose by causing premature tip stallingand longitudinal instability at high angles of attack andthus making it impossible for the airplane to attain its
maximum lift coefficient in flight. A model of a tail-
less all-wing airplane with sweepback and taper recentlytested in the Langley free-flight tunnel (reference 2)
showed this tendency. The maximum trim lift coefficient
CONFIDENTIAL
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CONFIDENTIAL NACA ACR No. L5G23
of this model with flaps retracted, as measured by forcetests, was about 1.2; tut because of the poor stability
and control near the stall the highest lift coefficientat which it could be flown was 0.7.
In an attempt to improve the longitudinal stabilitycharacteristics of swept-back all-wing tailless airplanes,an investigation of various means of preventing tip stallhas been made in the Langley free-flight tunnel. Themodel used in the tests of reference 2 was also used for
the present investigation. The test program includedforce and tuft tests, power off, of the original wing,
of the original wing with the wing tips rotated for wash-out, of the wing with modified rectangular and swept-forward wing tips , and of the original wing with fourslat arrangements. Flight tests were made with the origi-
nal wing and with the original wing equipped with themost promising modifications.
SYMBOLS
L lift, pounds
M pitching moment, foot-pounds
N yawing moment, pounds
C"L
/T
.
ft\lift coefficient i==-^)
\qsy
Cm pitching-moment coefficient about 0.20c
/pitching moment\ qcs
C-p, drag coefficientqa
S wing area, square feet
R Reynolds number
c wing chord, feet
mean aerodynamic chord, feet
CONFIDENTIAL
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NACA ACR No. L5C-23 CONFIDENTIAL 3
b wing semi span, feet
V airspeed, feet per second
a angle of attack, degrees
\J/angle of yaw, degrees
(3 angle of sideslip, degrees
angle of bank, degrees
rotation. of wing tip, degrees
6e
eleven deflection, degrees
5rrudder deflection, degrees
q dynamic pressure, pounds per square footj—pV
P mass density of air, slugs per cubic foot
APPARATUS
The tests were conducted in the Langley free-flighttunnel, which is described in reference 3- A photographof the test section of the tunnel showing the model in
flight is presented as figure 1.
Force tests made to determine the static stabilitycharacteristics
ofthe
model were made onthe
Langleyfree-
flight tunnel six-component balance. (For a descriptionof the balance see reference I|_.) All forces and momentsmeasured on this balance are taken with respect to the
stability axes, which are shown in figure 2.
The model is the one that was used in the tests
reported in reference 2. The model is of a tailless all-
wing airplane having an aspect ratio of 7-56, a taperratio (ratio of tip chord to root chord) of 0.23, and
sweepiback cf the quarter-chord line of 22°. A three-view
drawing of the model is presented as figure 3; a^d plan-view and three-quarter front-view photographs are pre-sented as figures I|. and 5 > respectively. For the present
CONFIDENTIAL
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k CONFIDENTIAL NACA AGR No. L5G23
tests , the wing tips were cut at the outboard end of the
elevens and altered so that the angle of incidence of the
tips could be changed or the tips removed entirely. (See
fig. 6.) Two additional sets of tips extending 28 percentof the wing semi span - one rectangular and one with 5°
sweepforward of the quarter- chord line - were built to
fit the wing where the original tips were cut. Leading-edge slats for the outer part of the span were constructedin three sections, any of which could be attached to the
wing separately.
The model tested in the Langley free -flight tunnel(designated PPT) at low Reynolds numbers was, in its
original condition, identical in plan form to a modelthat was tested in the Langley 19-foot pressure tunnel(designated 19-ft PT) at high Reynolds numbers; data forthe tests in the Langley 19-foot pressure tunnel are
given in the present paper for comparison with the resultaof tests in the Langley free-flight tunnel. The two
models, however, differed in airfoil section and numberof propeller-shaft housings. The model tested in the
Langley 19-foot pressure tunnel had an NACA 65(318 )-019
airfoil section at the root and NACA 65(318 )-015 section
at the tip; and the model tested in the Langley free-flight tunnel had a modified NACA 103 airfoil sectionwith a thickness of 21 percent chord at the root and
15 percent chord at the tip. The aerodynamic washout for
both models was approximately l\P
TESTS
Force tests were made to determine the static sta-
bility characteristics of the model in each of the testconditions. The force-test data for each arrangementwere based on the area and the mean aerodynamic chord of
the particular wing plan form tested.
Tuft studies were made of each model configurationto determine the stalling characteristics of the wing.For these tests, the model was mounted on the balancestrut
Force and tuft tests were run at a dynamic pressureof ko09 pounds per square foot, which corresponds to a
test Reynolds number of about 2l|.0,000 based on a mean
CONFIDENTIAL
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NACA ACR No. L5G23 CONFIDENTIAL 5
aerodynamic chord of 0.655 foot. All force and tuft
tests were made with flaps retracted, vertical fins off,
and the elevon and rudder control surfaces set at 0°.
Flight tests were made with combinations of slats 1
and 2 and 1, 2, and 3- (See fig. 6.) These testa- weremade with the center of gravity at 20 percent of the meanaerodynamic chord and over a range of lift coefficientsfrom 0.5 to 1.0. All flight tests were made with flaps,
retracted and with vertical fins installed. These finswere added to improve the directional stability; previoustests have indicated that they had no effect on longitu-dinal stability.
All tests were made with power off and propellersremoved.
RESULTS AND DISCUSSION
In interpreting the results of the tests made inthe Langley free-flight tunnel, the following pointsshould be considered:
(1) The tests were made at very low Reynolds numbers(150,000 to 350,000) .
(2) The controls of the model during the flighttests were fixed except during control applications;hence, no indication of the effect of the modificationson the control-free stability of the design was obtained.
Results of the force tests are shown in figure "]
In figure 8, the curves of pitching-moment coefficientagainst lift coefficient are replotted to compare the
stability characteristics for the various wing modifica-tions. Data for the model of similar plan form testedat high Reynolds numbers in the Langley 19-foot pressuretunnel are also shown in figures 7 and 8° Results of
tuft surveys in the Langley free-flight and 19-foot pres-
sure tunnels are presented in figure 9-
Original Wing
The force-test data of figure 8(a) and the tuft-testdata of figure 9( a ) illustrate the usual effect of
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6 CONFIDENTIAL NACA ACR No. L5G2J
sweepback and taper upon the static longitudinal stabilityand the stalling characteristics of a wing. These data
show that the premature stalling over the elevens nearthe wing tip caused the original wing to become neutrallystable at a lift coefficient of about 0.90.
The data of figures 7 an(i 8(h) also show that at
high lift coefficients the longitudinal instability of
the free-flight-tunnel model, tested at low Reynolds num-bers, was greater than that of the pressure-tunnel model,tested at high Reynolds numbers. The results of the
force tests made in the Langley free-flight tunnel are
believed to be conservative in that the necessary improve-
ment in longitudinal stability at high Reynolds numbersis less than the improvement indicated by the tests at
low Reynolds numbers. It is interesting to note, however,that in contrast to the dissimilarity of the pitching-moinent curves for the free-flight-tunnel model and the
pressure-tunnel model (fig. 8(h)), the stalling charac-
teristics as indicated by tuft surveys are quite similarfor the two models (figs. 9( a ) an(3 9(i))» When flown,
the model showed a tendency to nose-up and stall afterdisturbances in pitch at a lift coefficient of about 0.65>
and it was not possible to fly the model at lift coeffi-cients above 0.7. (See reference 2.)
Effect of Wing-Tip Modifications
A comparison of the curves in figure 8(a) shows that
rotating the wing tips -10° had little effect on the
longitudinal stability and did not prevent instabilityat the stall. The tuft-survey results in figures 9( a
)
and 9(b) show that, although the stalling of the tip was
improved slightly by deflecting the tip, the stall inboardof the tip was relatively unaffected. Correlation of
these results with force-test results indicates- that an
improvement of the stall over the elevons as well as overthe tips is necessary to eliminate the longitudinal insta-bility at high angles of attack.
Force tests of the swept-forward and rectangulartips (figs. 8(b) and 8(c)) showed no Improvement in the
stalling characteristics.
CONFIDENTIAL
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NACA ACR No. L5G23 CONFIDENTIAL
Effect of Slats
Addition of various slat arrangements caused definiteimprovements in the longitudinal stability characteristicsat the higher lift coefficients. This effect is shown infigures 8(d) to 8(g). The tuft tests showed that at highangles of attack the slat arrangements cleared the stallingon the tip in approximately direct proportion to the spanof the slats, and the premature stalling over the elevonswas improved only by the slat arrangements that extendedin front of the elevons. (See figs, 9(e) to 9(h).) Theslight roughness and stalling within the span of combina-
tions of slats 1 and 2 and 1, 2, and 3 is attributed toslat supports, which are located between the individualslats
With the 50 -5-percent- semi span slat and the 70 !?-
per cent-semi span slat installed, the model could be flownto a maximum lift coefficient of 1.0 - an increase of 0.3over the maximum lift coefficient with the original wing -
and did not show the nosing-up tendency noted In flighttests of the original wing.
CONCLUSIONS
The following conclusions were drawn from tests of
a tailless all-wing airplane model with various wingmodifications in the Lang ley free-flight tunnel:
1. Changes in wing-tip plan form over the outer28 percent of the wing semispan caused no appreciable
improvement in longitudinal stability at the stall.
2. Decreasing the angle of incidence of the wing' tip
(28 percent of the wing semispan) by 10° had little effecton the longitudinal stability and did not prevent longi-tudinal instability at the stall.
3. The use of partial-span wing slats eliminated the
longitudinal instability at the stall when the slat span
CONFIDENTIAL
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8 CONFIDENTIAL NACA ACR No. L5&23
was great enough to extend Inboard in front of the partof the wing that tended to stall first.
Langley Memorial Aeronautical LaboratoryNational Advisory Committee for Aeronautics
Langley Field, Va.
REFERENCES
1. Pitkin, Marvin, and Maggin, Bernard; Analysis of Fac-tors Affecting Net Lift Increment Attainable withTrailing-Edge Split Flans on Tailless Airplanes.NACA ARR No. lJj.118, I9J44.
2. Campbell, John P., and Seacord, Charles L., Jr.:Determination of the Stability and Control Charac-teristics of a Tailless All-Wing Airplane Modelwith Sweepback in the Langley Free-Flight Tunnel.
NACA ACR No. L5A13 , I9I4.5
3- Shortal, Joseph A., and Osterhout, Clayton J.: Pre-
liminary Stability and Control Tests in the NACAFree-Flight Wind Tunnel and Correlation with Full-Scale Flight Tests. NACA TN No. 810, I9J+I.
[).. Shortal, Joseph A., and Draper, John W.: Free-Flight-Tunnel Investigation of the Effect of the Fuselage
Length and the Aspect Ratio and Size of the VerticalTail on Lateral Stability and Control. NACA ARRNo. 3D17, 19^3.
CONFIDENTIAL
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Fig. 7 NACA ACR No. L5G23
Or/gina/ wing
Original lip (deflected -/0°)
Tip x? (swept forward)
Tip 3 (reclangular)^ Original wing J9-fl PT
Angle of alloc)cr , deg
20 ./
Pilehing-momenlcoefficient Cm
Figure 7- Aerodynamic characteristics of Lang/ey free-
fhghl - funnel ladless airplanemodel
wd/i var/ous wing
modifications. de = dr =0°; flaps relraded cenler-of-gravily locahon , 0.20 AA.A.C.
; q- 4.09 pounds per square
Idol excepl as noled.
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NACA ACR No. L5G23 Fig. 7 Cone.
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Fig. 8a-h NACA ACR No. L5G23
Original wing(alt plots)
(a)
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(b)
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,
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Figure 3.- Pilching-moment characler/slics of Iangley free-
flighl- tunnel fail/ess airplane model win various wingmodifications. cL=or
--0°J
flaps retracted center-of-gravity
location ,0.20MAC.,q= 4.09 pounds per square loot except
as noted.
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NACA ACR No. L5G23 Figc 9a,
CONFIDENTIAL
a(cleg)
(a) Original wing. (b) 8 = -10°.
12
16
20
Figure 9.- Results of tuft surveys of tailless airplane model In
Langley free-flight tunnel. 6e
= 6r = = 0°; q = 4.09 pounds
per square foot. NAT|0NAL mmmCONFIDENTIALCOMMITTEE FOR AERONAUTICS
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Fig. 9c, d NACA ACR No. L5G23
CONFIDENTIAL
(cleg)(C) Tip 2 (d)
Tip 3
Hough
12
16
20
Figure 9.- Continued.
CONFIDENTIAL
NATIONAL ADVISORY
COMMITTEE FOR AERONAUTICS
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NACA ACR No. L5G23 Fig. 9e,f
CONFIDENTIAL
a
(deg)(e) 31at 1 (f) Slat 2
L£X
12
16
20
Figure 9.- Continued.
CONFIDENTIAL
NATIONAL ADVISORY
COMMITTEE FOR AERONAUTICS
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Fig. 9g,h NACA ACR No. L5G23
CONFIDENTIAL
a
(deg) (g) Slats1and 2. (h) Slats 1, 2, and 3.
Rough Rough
12
16
20
Figure 9.- Continued.
CONFIDENTIAL
NATIONAL ADVISORY
COMMITTEE FOR AERONAUTICS
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NACA ACR No. L5G23 Fig. 9a,
CONFIDENTIAL
(deg) (a) Original wing, FFT.(i) Original wing, 19-ft PT.
R = 6.6 x 106.
Rough
12
16
Figure 9.- Concluded.
CONFIDENTIAL
NATIONAL ADVISORY
COMMITTEE FOR AERONAUTICS
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