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Subsonic Wingsan introduction
W.H. Mason
Configuration Aerodynamics Class
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VLM Methods – a way to get insight
•
Linear, inviscid aerodynamics – strictly subsonic
• Ignores thickness – bc’s applied on the mean plane
– Finds !Cp, not the upper/lower surface pressures
• Very handy and accurate as seen below
• Really good for understanding interacting surface ideas
Choices: VLMpc, Tornado, AVL
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VLM Models and Tips
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Convergence with number of “panels”
F/A-18
0
2
4
0 40 80 120 160 200 240
Total number of panels
Vortex Lattice Method
(5) (9)
( ) Number of chordwise panels
! Neutralpoint,
percent c
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Panel Models
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F-15 3-Surface VLM Model
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Three-Surface F-15 Longitudinal Derivatives
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Canard Height Effect
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F-15 horizontal tail effectiveness
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F-15 aileron effectiveness
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Warren-12 Test Case
Note: C M about wing apex,
Reference chord is 1.0
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The key:
Define it for
others!
Thereference
trap wing
Source: Stinton, Design of the Airplane
Comment: Reference Area(s)
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Aerodynamics of High Aspect Ratio Wings
• Planforms
• Spanloads
• Pitching moment and pitchup
• Aerodynamic Center
• Isobars/Twist
• Camber
• 2D-3D connection
• Canard and Ground Effects
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Typical Planform Characteristics of
Transport Aircraft
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Clearly the A380 pays a price to satisfy the 80 meter gate box limit
Way offthe trend
line!
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Forward, Unswept and Aft Swept Planforms, AR = 2.8
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Related Spanloads and Section Lift Coefficients
0.00
0.20
0.40
0.60
0.80
1.00
1.20
1.40
1.60
0.0 0.2 0.4 0.6 0.8 1.0y/(b/2)
Spanload,
Warren 12 planform, sweep changed
aft swept wing
unswept wing
forward swept wing
ccl / c
a
0.00
0.20
0.40
0.60
0.80
1.00
1.20
1.40
0.0 0.2 0.4 0.6 0.8 1.0
y/(b/2)
Section CL
Warren 12 planform, sweep changed
aft swept wing
unswept wing
forward swept wing
For an untwistedplanar wing
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Forward, Unswept and Aft Swept Planforms, AR = 8
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Related Spanloads and Section Lift Coefficients
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
0.0 0.2 0.4 0.6 0.8 1.0
Spanload,
y/(b/2)
Aspect ratio 8 wings
aft swept wing
unswept wing
forward swept wing
ccl / c
a
0.00
0.50
1.00
1.50
0.0 0.2 0.4 0.6 0.8 1.0
Section CL
Aspect ratio 8 planforms
aft swept wing
unswept wing
forward swept wing
y/(b/2)
For an untwistedplanar wing
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Example: VLM Pitching Moment agrees well
with data until wing pitchup
-0.06
-0.04
-0.02
0.00
0.02
0.04
0.06
0.08
-0.4 -0.2 0.0 0.2 0.4 0.6 0.8 1.0 1.2
C m
C L
AR = 10, !c/4 = 35°, " = 0.5
data from NACA RM A50K27
Re = 10 million
x ref = c/4
VLMpc calculation
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Aerodynamic Center on Finite Wings
- is it actually at the quarter chord? -
From Shevelle, Fundamentals of Flight , 2
nd
Ed.
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Low Aspect Ratio Wing Neutral Point (ac )For a rectangular wing it moves forward!
From Schlichting and Truckenbrodt,
Aerodynamics of the Airplane
AR
Discovered while making
pre-test estimates
Inboard Wing built/tested at VT
0.25
0.05
1
5 7
3
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Isobars
Note: this is actually a transonic case, M = 0.93, ! = 2°from AFFDL-TR-77-122, February 1978.
These funny NACA report numbers
denote series classified at the time,
“L” stands for Langley, reportsstarting with “A” denote Ames
Without twist and camber: don’t get full effect of sweep
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Typical Twist Distributions
-1.0
0.0
1.0
2.0
3.0
4.0
5.06.0
7.0
0 0.2 0.4 0.6 0.8 1
! ,
deg.
y/(b/2)
-1.0
0.0
1.0
2.0
3.0
4.05.0
6.0
0 0.2 0.4 0.6 0.8 1
! ,
deg.
y/(b/2)
Aft Swept Wing Forward Swept Wing
from LAMDES on the software website
A LAMDES artifact
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Typical Camber Variation
-0.01
0.00
0.01
0.02
0.03
0.04
0.05
-0.2 0 0.2 0.4 0.6 0.8 1 1.2
(z-zle)/c
x/c
! = 0.925
! = 0.475
! = 0.075
Cambers from the LAMDES code on the software website
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Relating 2D and 3D
The airfoil problem is converted to 2D (normal),
solved (designed), and put in the wing 3D
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Canard-Wing Interaction
canard wake extends to indinitywing wake not shown
A A
Canard wakestreams overwing
-2.0-1.5-1.0-0.50.0
0.51.01.5
-2 -1.5 -1 -0.5 0 0.5 1 1.5 2
w
Downwash from canard across wingat Section A-A
Upwash outboardof canard tips
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Example for Minimum Induced Drag
Calculations
Sample case in John Lamar’s NASA TN with LAMDES
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Canard Wing Induced Drag
0.0200
0.0250
0.0300
0.0350
0.0400
-0.4 -0.3 -0.2 -0.1 0.0 0.1 0.2 0.3 0.4
C Di
!x/cForward Aft
Canard lift must benegative to trim
M = 0.3, C L
= 0.5
Canard heightabove wing ,
0.1
0.2
z/b
0.3
Computations from LamDes
Advantage of verticalseparation clearly evident
Static Margin
Stable Unstable
Advantage of relaxedstatic stability evident
Note: The sample case may not be a gooddesign, the canard is too big.
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Typical Required Twist Distribution
-1.0
0.01.0
2.0
3.0
4.0
5.0
6.0
0.0 0.2 0.4 0.6 0.8 1.0
! ,
y/(b/2)
in presenceof canard
without
canard canard tipvortex effect
deg.
-2.0
0.0
2.0
4.0
6.0
8.0
0.0 0.2 0.4 0.6 0.8 1.0
!
y/(b/2)
withoutcanard
in presenceof canard
canard tip
vortex effect
Aft Swept Wing
Forward Swept Wing
Actual twist values are heavily
dependent on the canard load!
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Some Variations: Tip treatment
from Feifel, in NASA SP-405, 1976
A Whitcomb “winglet”
The “Raked Wingtip” used
on the Boeing 767-400
from Kroo, Ann. Rev. of Fluid Mech., 2001
Rounding the intersection
leads to a “blended winglet”
Note “Yehudi”
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Ground Effects from VLM
1.0
2.0
3.0
4.0
5.0
6.0
7.0
8.0
0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4
C L!
h/c
AR
4
2
1
Solid lines: computed using JKayVLMDashed lines: from Kalman, Rodden and GiesingSymbols: Experimental data
h
U !
c
c/4
-0.40
-0.30
-0.20
-0.10
0.00
0.10
0.20
0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4
C M !
h/c
Solid lines: computed using JKayVLMDashed lines: from Kalman, Rodden and Giesing
AR1
2
4
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A completely new category
Slender Wings
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Laser Light Sheet Leading Edge Vortex Flow
Aviation Week & Space Technology, July 29, 1985
Light Sheet is a
great way to see
the LE vortex
Northrop IR & D
example of flow
over a delta wing
configuration.
Exhibited at the
36th Paris airshow.
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Vortex Lift
Drawback?
It’s “draggy” lift
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The Polhamus LE Suction Analogy
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Another View of the Suction Analogy
R.M. Kulfan, Wing Geometry Effects on Leading Edge Vortices, AIAA 79-1872
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Results of the Polhamus Suction Analogy
0.00
0.500
1.00
1.50
2.00
0.0° 10.0° 20.0° 30.0° 40.0°
CL
!
AR = 1.5 ("
= 69.4°)
VortexLift
PotentialLift
Experimental data fromBartlett and Vidal
Prediction from PolhamusLeading Edge Suction Analogy
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Reduce Drag with a Vortex Flap ?
The Concept
The reality?
Flight International, 16 March 1985
This concept was briefly popular,
but it proved too hard to achieve.
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Strakes are also low aspect ratio wings. Because they
don#t stall, even low tail designs can have
a nose-down moment problem
F-16
Forebody
Strakes
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The Concorde Exploited Both Ground Effects
and Vortex Lift to be Even Somewhat Practical
From Poisson-Quinton, Sustained Supersonic Cruise Aircraft Experience
Vortex
Burst
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And VLM works for Hypersonic Class Concepts
Jimmy Pittman and James Dillon, “Vortex Lattice Prediction of Subsonic
Aerodynamics of Hypersonic Vehicle Concepts,” Journal of Aircraft ,
October 1977, pp. 1017-1018.
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To Conclude
This just gives you the very basics
- no end to planform concepts, invent one yourself!