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ME403 Chapter 2 2D Airfoil Aerodynamics Lift is mainly provided by the wing with an airfoil cross-section shape

ME403 Chapter 2 2D Airfoil Aerodynamics

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ME403 Chapter 2 2D Airfoil Aerodynamics. Lift is mainly provided by the wing with an airfoil cross-section shape. Airfoil Geometry. An airfoil is the 2D cross-section shape of the wing, which creates significant lift but minimal drag because of this aerodynamic shape. Historical Airfoils. - PowerPoint PPT Presentation

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Page 1: ME403 Chapter 2 2D Airfoil Aerodynamics

ME403 Chapter 22D Airfoil Aerodynamics

Lift is mainly provided by the wing with an airfoil

cross-section shape

Page 2: ME403 Chapter 2 2D Airfoil Aerodynamics

Airfoil Geometry

An airfoil is the 2D cross-section shape of the wing,

which creates significant lift but minimal drag because of

this aerodynamic shape

Page 3: ME403 Chapter 2 2D Airfoil Aerodynamics

Historical Airfoils

Page 4: ME403 Chapter 2 2D Airfoil Aerodynamics

Historical Airfoils

Page 5: ME403 Chapter 2 2D Airfoil Aerodynamics

Typical Streamlines

Angle of Attack

chord lineV

Page 6: ME403 Chapter 2 2D Airfoil Aerodynamics

Pressure Distribution

99500

99550

99600

99650

99700

99750

99800

99850

99900

99950

100000

0 0.2 0.4 0.6 0.8 1

Chordwise Distance, x, m

Su

rfa

ce P

ress

ue

, P, N

/sq

m

Net Normal Force

Upper Surface Pressure

Lower Surface Pressure

n P P dxl

c

u ( )0

Page 7: ME403 Chapter 2 2D Airfoil Aerodynamics

Pressure Coefficient Distribution

02

2

1

V

ppcp

2

2

1

V

ppcp

In the uniform free-stream:

At the stagnation point

(at which velocity V=0): 12

2

1

2

2

1

2

2

10

0

V

V

V

ppcp

Positive Cp means the pressure is higher than the free-stream (atmospheric) pressure, and negative Cp means suction relative to free-stream pressure. The maximum, which occurs at the stagnation point, is always 1.

Page 8: ME403 Chapter 2 2D Airfoil Aerodynamics

Viscous Boundary Layer

Transition Separation

1 23

4

V Edge of boundary layer

Velocity profile creates skin friction (shear) drag on surface

Page 9: ME403 Chapter 2 2D Airfoil Aerodynamics

Curve fit formula for turbulent boundary layer (Re > 500,000):

Flat Plate Skin Friction Drag Coefficient

Page 10: ME403 Chapter 2 2D Airfoil Aerodynamics

Evolution of Airfoil Design

Delaying transition point from Laminar to Turbulent boundary layer reduces skin

friction drag

Page 11: ME403 Chapter 2 2D Airfoil Aerodynamics

Boundary Layer Flow Separation

When flow separation occurs, there is also pressure drag.

Page 12: ME403 Chapter 2 2D Airfoil Aerodynamics

100% Pressure Drag

Pressure (Form) Drag due to Flow Separation

Total Profile Drag= Skin Friction Drag

+ Form Drag

Page 13: ME403 Chapter 2 2D Airfoil Aerodynamics

Resultant Aerodynamic Force

Airfoil

Total Aerodynamic Force(Sum of Pressure and Shear)

Lift

Drag

V

Page 14: ME403 Chapter 2 2D Airfoil Aerodynamics

Lift & Drag Coefficients

Chord Line

normal forcelift

V

drag

chordwise force

cV

l

cbV

Lcl 2

2

12

2

1

cV

d

cbV

Dcd 2

2

12

2

1

Page 15: ME403 Chapter 2 2D Airfoil Aerodynamics

Center of PressureThe resultant aerodynamic force acts at the Center of

Pressure (c.p.), about which the moment is zero.

Page 16: ME403 Chapter 2 2D Airfoil Aerodynamics

Open-Circuit Wind Tunnel

Page 17: ME403 Chapter 2 2D Airfoil Aerodynamics

Wind Tunnel Tests

Force transducer behind model senses lift, drag and pitching moment directly.Motor-controlled mechanism adjusts the model’s angle of attack.

Page 18: ME403 Chapter 2 2D Airfoil Aerodynamics

Closed-Circuit Wind Tunnel

Page 19: ME403 Chapter 2 2D Airfoil Aerodynamics

Wing Section Models

Model for measuring lift, drag and pitching moment

Model for measuring surface pressure distribution

Page 20: ME403 Chapter 2 2D Airfoil Aerodynamics

There is a maximum Lift-to-Drag ratio (L/D).

Location of Center of Pressure (c.p.) varies

with

NACA 0006 Dataat Re = 3,180,000

Page 21: ME403 Chapter 2 2D Airfoil Aerodynamics

NACA 2312 Data at Re = 3,120,000

Lift decreases and drag increases sharply beyond the stall (max. Cl) point, due to boundary layer separation.

Page 22: ME403 Chapter 2 2D Airfoil Aerodynamics

NACA Airfoils and Test Data

4-Digit Series

5-Digit Series

6 Series

http://naca.larc.nasa.gov/reports/1945/naca-report-824/

Page 23: ME403 Chapter 2 2D Airfoil Aerodynamics

Stalled Airfoil

Page 24: ME403 Chapter 2 2D Airfoil Aerodynamics

Reynolds Number Effect

Page 25: ME403 Chapter 2 2D Airfoil Aerodynamics

Since the c.p. varies with , it is more desirable to use a fixed Aerodynamic Center (a.c.) as the point of action of the lift and drag. The pitching moment about this point can be calculated, and is found insensitive to . For most

airfoils, the a.c. locates at around quarter chord (x=c/4).

Aerodynamic Center

222

1 cV

mcm

Pitching Moment Coefficient:

Page 26: ME403 Chapter 2 2D Airfoil Aerodynamics

Typical Non-Cambered AirfoilLift Curve & Drag Polar

NACA 0006

Page 27: ME403 Chapter 2 2D Airfoil Aerodynamics

Typical Cambered AirfoilNACA 2412

Lift Curve & Drag Polar

Page 28: ME403 Chapter 2 2D Airfoil Aerodynamics

Typical Airfoil Aerodynamic Characteristicsat Re = 6 million

NACA 0006 NACA 2412

Zero-Lift Angle of Attack (deg.) 0 -2

Stall Angle of Attack (deg.) 9 16

Maximum Lift Coefficient 0.9 1.7

Lift Curve Slope (/deg.) 0.1 0.108

Moment Coefficient (before stall) 0 -0.05 to -0.02

Minimum Drag Coefficient 0.005 0.006

Max. Lift-to-Drag Ratio (L/D) 0.7/0.0076 = 92.1 1.0/0.0088 = 113

Page 29: ME403 Chapter 2 2D Airfoil Aerodynamics

Computation Fluid Dynamics Simulation

Page 30: ME403 Chapter 2 2D Airfoil Aerodynamics

CFD Simulation: Near stall

Page 31: ME403 Chapter 2 2D Airfoil Aerodynamics

CFD Simulation: Fully Stalled

Page 32: ME403 Chapter 2 2D Airfoil Aerodynamics

Airfoil Generator at http://www.ae.su.oz.au/aero/info/index.html

Page 33: ME403 Chapter 2 2D Airfoil Aerodynamics

Airfoil Analysis Code at http://www.ae.su.oz.au/aero/info/index.html