Lift coefficient.html

A typical lift coefficient curve.

The lift coefficient (C_L or C_Z) is a non-dimensional coefficient that relates the lift generated by an airfoil, the dynamic pressure of the fluid flow around the airfoil, and the planform area of the airfoil.^[1]^[2] It may also be described as the ratio of lift pressure to dynamic pressure.

Lift coefficient may be used to relate the total lift generated by an aircraft to the total area of the wing of the aircraft. In this application it is called the aircraft lift coefficient C_L.

The lift coefficient C_L is equal to:^[3]^[2]

$C_L={L \over \frac{1}{2}\rho v^2A} = \frac{L}{q A}$
where

L is the lift force,
ρ is fluid density,
v is true airspeed,
q is dynamic pressure, and
A is planform area.

The lift coefficient can be approximated using the Thin Airfoil Theory or Lifting-line theory.

Lift coefficient may also be used as a characteristic of a particular shape (or cross-section) of an airfoil. In this application it is called the section lift coefficient c_L. It is common to show, for a particular airfoil section, the relationship between lift coefficient and angle of attack.^[4] It is also useful to show the relationship between lift coefficient and drag coefficient.

The section lift coefficient is based on the concept of an infinite wing of non-varying cross-section. It is not practical to define the section lift coefficient in terms of total lift and total area because they are infinitely large. Rather, the lift is defined per unit span of the wing (L'). In such a situation, the above formula becomes:

$c_L={L' \over \frac{1}{2}\rho v^2c}$

where c is the chord length of the airfoil.

Note that the lift equation does not include terms for angle of attack — that is because there is no mathematical relationship between lift and angle of attack. (In contrast, there is a straight-line relationship between lift and dynamic pressure; and between lift and area.) The relationship between the lift coefficient and angle of attack is complex and can only be determined by experimentation or complex analysis. See the accompanying graph. The graph for section lift coefficient vs. angle of attack follows the same general shape for all airfoils, but the particular numbers will vary. The graph shows an almost linear increase in lift coefficient with increasing angle of attack, up to a maximum point, after which the lift coefficient falls away rapidly. This indicates the lift coefficient at the stall of the airfoil.

The lift coefficient is a dimensionless number.

Note that in the graph here, there is still a small but positive lift coefficient with angles of attack less than zero. This is true of any airfoil with camber (asymmetrical airfoils). On a cambered airfoil at zero angle of attack the pressures on the upper surface are lower than on the lower surface.

References

Clancy, L.J. (1975), Aerodynamics, Pitman Publishing Limited, London ISBN 0 273 01120 0
Abbott, Ira H., and Von Doenhoff, Albert E. (1959), Theory of Wing Sections, Dover Publications Inc., New York, Standard Book Number 486-60586-8

Notes

^ Clancy, L.J., Aerodynamics, Sections 4.15 and 5.4
^ ^a ^b Abbott, Ira H., and Von Doenhoff, Albert E., Theory of Wing Sections, Section 1.2
^ Clancy, L.J., Aerodynamics, Section 4.15
^ Abbott, Ira H., and Von Doenhoff, Albert E., Theory of Wing Sections, Appendix IV

Lift coefficient.html

References

Notes

See also