UNIT - VII Aerodynamic Characteristics of Airfoils and

UNIT - VII Aerodynamic Characteristics of Airfoils and

UNIT - VII Aerodynamic Characteristics of Airfoils and wings Aerodynamic forces and Moments

coefficients Aerodynamic forces Aerodynamic forces exerted by airflow comes from only two sources

Pressure, p, distribution on surface Acts normal to surface Shear stress, tw, (friction) on surface

Acts tangentially to surface Pressure and shear are in units of force per unit area (N/m2) Net unbalance creates an aerodynamic force

No matter how complex the flow field, and no matter how complex the shape of the body, the only way nature has of communicating an

aerodynamic force to a solid object or surface is through the pressure and shear stress distributions that exist on the surface.

The pressure and shear stress distributions are the two hands of nature that reach out and grab the body, exerting a force on the body the aerodynamic force

Aerodynamic forces and moments are due to Pressure distribution Shear stress distribution

Nomenclature R resultant force L lift D drag

N normal force A Axial force Relative Wind: Direction of V

We used subscript to indicate far upstream conditions Angle of Attack, a: Angle between relative wind (V) and chord line Total aerodynamic force, R, can be resolved into two force

components Lift, L: Component of aerodynamic force perpendicular to relative wind Drag, D: Component of aerodynamic force parallel to relative wind

Center of Pressure: It is that point on an airfoil (or body) about which the aerodynamic moment is zero Aerodynamic Center: It is that point on an airfoil (or body) about

which the aerodynamically generated moment is independent of angle of attack Moments About Leading Edge , quarter Chord point and about

center of pressure Center of Pressure: It is that point on an airfoil (or body) about which the aerodynamic moment is zero

Thin Airfoil Theory: Symmetric Airfoil: Cambered Airfoil:

c 4 c

xcp 1 A1 A2 4 cl xcp

Aerodynamic Center: It is that point on an airfoil (or body) about which the aerodynamically generated moment is independent of angle of attack Thin Airfoil Theory:

Symmetric Airfoil: Cambered Airfoil: x A.C .

x A.C . c

4 c 4

Drag Polar Drag Polar : both the Cl and Cd are the

functions of angle of attack thus the drag coefficient is that it depends on lift coefficient and the typical variations on Cl and Cd is called as Drag polar

The Drag polar is very important in performance analysis of aircrafts. For an aircraft with symmetrical airfoil sections the drag polar is given as CD = CDO+KCL2

Lift Curve Slope Lift Curve Slope

Lift Curve for a Normal Wing and NACA 63415 Wing Lift curve for High aspect ratio wing and Delta wing Aircraft

Lift curve for a straight wing and Swept wing Aircraft Maximum Lift Coefficient

Lift coefficient changes with addition of control surfaces Lift coefficient changes with increase in aspect ratio and

also Angle of attack can be decreased Lift coefficient increasing with maximum thickness

Variation of Cl, CD, L/D with AOA Increase in lift coefficient with different control

surfaces or high lift devices Minimum drag coefficient

To obtain minimum drag coefficient 1) we have to streamline the body

2) Increasing the sweep angle Drag coefficient data obtained for a rectangular wing and swept back wing on wing tunnel and lifting line numerical methods

Min drag coefficient for wing section and complete airplane

It gives the maximum possible glide angle Max values of L/D ratios

Effect of Airfoil and wing geometry Airfoil Nomenclature

Reynolds No, Boundary Layer Transition and surface roughness NACA Conventional Airfoils

Laminar Flow Airfoils An airfoil designed for minimum drag

and uninterrupted flow of the boundary layer is called a laminar airfoil. Supercritical Airfoils:

Designed to delay and reduce transonic drag rise, due to both strong normal shock and shock-induced boundary layer separation

Whitchomb supercritical airfoils Drag Reduction And lift Augmentation Methods

Many theories have been developed on how a wing generates lift. The most common one is the Longer Path Theory.

This theory describes how the shape of the aerofoil produces a pressure difference which generates lift. As the aerofoil is designed in such a way that its upper surface is longer than the bottom, and because the molecules that hit the leading edge must meet again at the trailing edge, the ones that travel on the upper surface do so with

greater velocity than the lower Flap system Leading edge devices

Multi element airfoils Circulation control Laminar flow control winglets

Flap systems Flap is an element attached to the aileron

of the wing section It is always possible to reduce stall speed by increasing wing area

Different types of flap system Flaps change the airfoil pressure distribution, increasing the camber of the airfoil and allowing more of the lift to be

carried over the rear portion of the section Leading Edge Devices

Leading Edge Devices Leading edge devices such as nose flaps, Kruger flaps, and slats reduce the pressure peak

near the nose by changing the nose camber. Slots and slats permit a new boundary layer to start on the main wing portion, eliminating the detrimental effect of the initial adverse gradient.

A Wing with slats and Flaps Multi Element Airfoils

Circulation Control Circulation Control Wing technology is one of the most important potential applications of the

Coanda Effect. The objective is to replace the lift devices on the leading and trailing edges of a wing by use of Coanda Surfaces and slot blowing instead.

Laminar Flow Control Winglets

Winglets

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