Kutta–Joukowski theorem

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The Kutta–Joukowski theorem is a fundamental theorem in aerodynamics used for the calculation of lift of an airfoil and any two-dimensional bodies including circular cylinders translating in a uniform fluid at a constant speed large enough so that the flow seen in the body-fixed frame is steady and unseparated. The theorem relates the lift generated by an airfoil to the speed of the airfoil through the fluid, the density of the fluid and the circulation around the airfoil. The circulation is defined as the line integral around a closed loop enclosing the airfoil of the component of the velocity of the fluid tangent to the loop.[1] It is named after the German Martin Wilhelm Kutta and the Russian Nikolai Zhukovsky (or Joukowski) who first developed its key ideas in the early 20th century. Kutta–Joukowski theorem is an inviscid theory, but it is a good approximation for real viscous flow in typical aerodynamic applications.

Kutta–Joukowski theorem relates lift to circulation much like the Magnus effect relates side force (called Magnus force) to rotation.[2] However, the circulation here is not induced by rotation of the airfoil. The fluid flow in the presence of the airfoil can be considered to be the superposition of a translational flow and a rotating flow. This rotating flow is induced by the effects of camber, angle of attack and a sharp trailing edge of the airfoil. It should not be confused with a vortex like a tornado encircling the airfoil. At a large distance from the airfoil, the rotating flow may be regarded as induced by a line vortex (with the rotating line perpendicular to the two-dimensional plane). In the derivation of the Kutta–Joukowski theorem the airfoil is usually mapped onto a circular cylinder. The theorem is proved in many text books for a circular cylinder and the Joukowski airfoil, but it holds true for general airfoils.

Lift force formula[edit]

The theorem applies to two-dimensional flow around a fixed airfoil (or any shape of infinite span). The lift per unit span of the airfoil is given by[3]

 

 

 

 

(1)

where and are the fluid density and the fluid velocity far upstream of the airfoil, and is the circulation defined as the line integral

around a closed contour enclosing the airfoil and followed in the positive (anti-clockwise) direction. As explained below, this path must be in a region of potential flow and not in the boundary layer of the cylinder. The integrand is the component of the local fluid velocity in the direction tangent to the curve and is an infinitesimal length on the curve, . Equation (1) is a form of the Kutta–Joukowski theorem.

Kuethe and Schetzer state the Kutta–Joukowski theorem as follows:[4]

The force per unit length acting on a right cylinder of any cross section whatsoever is equal to and is perpendicular to the direction of

Circulation and the Kutta condition[edit]

A lift-producing airfoil either has camber or operates at a positive angle of attack, the angle between the chord line and the fluid flow far upstream of the airfoil. Moreover, the airfoil must have a "sharp" trailing edge.

Any real fluid is viscous, which implies that the fluid velocity vanishes on the airfoil. Prandtl showed that for large Reynolds number, defined as , and small angle of attack, the flow around a thin airfoil is composed of a narrow viscous region called the boundary layer near the body and an inviscid flow region outside. In applying the Kutta-Joukowski theorem, the loop must be chosen outside this boundary layer. (For example, the circulation calculated using the loop corresponding to the surface of the airfoil would be zero for a viscous fluid.)

The sharp trailing edge requirement corresponds physically to a flow in which the fluid moving along the lower and upper surfaces of the airfoil meet smoothly, with no fluid moving around the trailing edge of the airfoil. This is known as the "Kutta condition."

Kutta and Joukowski showed that for computing the pressure and lift of a thin airfoil for flow at large Reynolds number and small angle of attack, the flow can be assumed inviscid in the entire region outside the airfoil provided the Kutta condition is imposed. This is known as the potential flow theory and works remarkably well in practice.

Derivation[edit]

Two derivations are presented below. The first is a heuristic argument, based on physical insight. The second is a formal and technical one, requiring basic vector analysis and complex analysis.

Heuristic argument[edit]

For a rather heuristic argument, consider a thin airfoil of chord and infinite span, moving through air of density . Let the airfoil be inclined to the oncoming flow to produce an air speed on one side of the airfoil, and an air speed on the other side. The circulation is then

The difference in pressure between the two sides of the airfoil can be found by applying Bernoulli's equation:

so the lift force per unit span is

A differential version of this theorem applies on each element of the plate and is the basis of thin-airfoil theory.

Formal derivation[edit]

Lift forces for more complex situations[edit]

The lift predicted by Kutta Joukowski theorem within the framework of inviscid potential flow theory is quite accurate even for real viscous flow, provided the flow is steady and unseparated.[6]

a) Kutta Joukowski Theorem for steady irrotational flow. In deriving the Kutta–Joukowski theorem, the assumption of irrotational flow was used. When there are free vortices outside of the body, as may be the case for a large number of unsteady flows, the flow is rotational. When the flow is rotational, more complicated theories should be used to derive the lift forces. Below are several important examples.

b) Impulsively started flow at small angle of attack. For an impulsively started flow such as obtained by suddenly accelerating an airfoil or setting an angle of attack, there is a vortex sheet continuously shed at the trailing edge and the lift force is unsteady or time-dependent. For small angle of attack starting flow, the vortex sheet follows a planar path, and the curve of the lift coefficient as function of time is given by the Wagner function.[7] In this case the initial lift is one half of the final lift given by the Kutta Joukowski formula.[8] The lift attains 90% of its steady state value when the wing has traveled a distance of about seven chord lengths.

c) Impulsively started flow at large angle of attack. When the angle of attack is high enough, the trailing edge vortex sheet is initially in a spiral shape and the lift is singular (infinitely large) at the initial time.[9] The lift drops for a very short time period before the usually assumed monotonically increasing lift curve is reached.

d) Starting flow at large angle of attack for wings with sharp leading edges. If, as for a flat plate, the leading edge is also sharp, then vortices also shed at the leading edge and the role of leading edge vortices is two-fold:(1) they are lift increasing when they are still close to the leading edge, so that they elevate the Wagner lift curve,(2) they are detrimental to lift when they are convected to the trailing edge, inducing a new trailing edge vortex spiral moving in the lift decreasing direction. For this type of flow a vortex force line (VFL) map [10] can be used to understand the effect of the different vortices in a variety of situations (including more situations than starting flow) and may be used to improve vortex control to enhance or reduce the lift. The vortex force line map is a two dimensional map on which vortex force lines are displayed. For a vortex at any point in the flow, its lift contribution is proportional to its speed, its circulation and the cosine of the angle between the streamline and the vortex force line. Hence the vortex force line map clearly shows whether a given vortex is lift producing or lift detrimental.

e) Lagally Theorem. When a (mass) source is fixed outside the body, a force correction due to this source can be expressed as the product of the strength of outside source and the induced velocity at this source by all the causes except this source. This is known as the Lagally theorem.[11] For two-dimensional inviscid flow, the classical Kutta Joukowski theorem predicts a zero drag. When, however, there is vortex outside the body, there is a vortex induced drag, in a form similar to the induced lift.

f) Generalized Lagally Theorem. For free vortices and other bodies outside one body without bound vorticity and without vortex production, a generalized Lagally theorem holds,[12] with which the forces are expressed as the products of strength of inner singularities (image vortices, sources and doublets inside each body) and the induced velocity at these singularities by all causes except those inside this body. The contribution due to each inner singularity sums up to give the total force. The motion of outside singularities also contributes to forces, and the force component due to this contribution is proportional to the speed of the singularity.

g) Individual force of each body for Multiple-body rotational flow. When in addition to multiple free vortices and multiple bodies, there are bound vortices and vortex production on the body surface, the generalized Lagally theorem still holds, but a force due to vortex production exists. This vortex production force is proportional to the vortex production rate and the distance between the vortex pair in production. With this approach, an explicit and algebraic force formula, taking into account of all causes (inner singularities, outside vortices and bodies, motion of all singularities and bodies, and vortex production) holds individually for each body [13] with the role of other bodies represented by additional singularities. Hence a force decomposition according to bodies is possible.

h) General three dimensional viscous flow. For general three-dimensional, viscous and unsteady flow, force formulas are expressed in integral forms. The volume integration of certain flow quantities, such as vorticity moments, is related to forces. Various forms of integral approach are now available for unbounded domain[8][14][15] and for artificially truncated domain.[16] The Kutta Joukowski theorem can be recovered from these approaches when applied to a two-dimensional airfoil and when the flow is steady and unseparated.

i) Lifting line theory for wings, wing tip vortices and induced drag. A wing has a finite span, and the circulation at any section of the wing varies with the spanwise direction. This variation is compensated by the release of streamwise vortices (called trailing vortices), due to conservation of vorticity or Kelvin Theorem of Circulation Conservation. These streamwise vortices merge to two counter-rotating strong spirals, called wing tip vortices, separated by distance close to the wing span and may be visible if the sky is cloudy. Treating the trailing vortices as a series of semi-infinite straight line vortices leads to the well-known lifting line theory. By this theory, the wing has a lift force smaller than that predicted by a purely two-dimensional theory using the Kutta–Joukowski theorem. Most importantly, there is an induced drag. This induced drag is a pressure drag which has nothing to do with frictional drag.

See also[edit]

Notes[edit]

  1. ^ Anderson, J.D. Jr., Introduction to Flight, Section 5.19, McGraw-Hill, NY (3rd ed. 1989.)
  2. ^ "Lift on rotating cylinders". NASA Glenn Research Center. 2010-11-09. Retrieved 2013-11-07. 
  3. ^ Clancy, L.J., Aerodynamics, Section 4.5
  4. ^ A.M. Kuethe and J.D. Schetzer, Foundations of Aerodynamics, Section 4.9 (2nd ed.)
  5. ^ Batchelor, G. K., An Introduction to Fluid Dynamics, p 406
  6. ^ Anderson J. Fundamentals of Aerodynamics, Mcgraw-Hill Series in Aeronautical and Aerospace Engineering, McGraw-Hill Education, New York 2010
  7. ^ Wagner H Uber die Entstehung des dynamischen Auftriebes von Tragflueln. Z. Angew. Math. Mech.1925, 5, 17.
  8. ^ a b Saffman PG Vortex Dynamics, Cambridge University Press, New York, 1992 .
  9. ^ Graham JMR,The lift on an aerofoil in starting flow |publisher= Journal of Fluid Mechanics, 1983, vol 133, pp 413-425
  10. ^ Li J, Wu ZN. "Unsteady lift for the Wagner problem in the presence of additional leading trailing edge vortices". Journal of Fluid Mechanics, 2015, Vol 769, pp 182 - 217. 
  11. ^ Milne-Thomson L M. Theoretical Hydrodynamics [p226], Macmillan Education LTD, Hong Kong.1968
  12. ^ Wu CT, Yang FL & Young DL Generalized two-dimensional Lagally theorem with free vortices and its application to fluid-body interaction problems, Journal of Fluid Mechanics, 2012, vol 698, pp73--92.
  13. ^ Bai CY, Li J, Wu ZN. "Generalized Kutta-Joukowski theorem for multi-vortex and multi-airfoil flow with vortex production — A general model". Chinese Journal of Aeronautics,2014 Vol.27(5), pp1037-1050. 
  14. ^ Wu JC, Theory for aerodynamic force and moment in viscous flows, AIAA Journal,1981, vol. 19, pp432-441.
  15. ^ Howe MS, On the force and moment on a body in an incompressible fluid, with application to rigid bodies and bubbles at high Reynolds numbers, Quartly Journal of Mechanics and Applied Mathematics, 1995,vol.48, pp401-425.
  16. ^ Wu JC, Lu XY & Zhuang LX, Integral force acting on a body due to local flow structures, Journal of Fluid Mechanics, 2007, vol.576, pp265-286.

References[edit]

  • Batchelor, G. K. (1967) An Introduction to Fluid Dynamics, Cambridge University Press
  • Clancy, L.J. (1975), Aerodynamics, Pitman Publishing Limited, London ISBN 0-273-01120-0
  • A.M. Kuethe and J.D. Schetzer (1959), Foundations of Aerodynamics, John Wiley & Sons, Inc., New York ISBN 0-471-50952-3