The aerodynamic forces on a body moving at constant velocity are the drag force D opposing the motion and the lift force L in the direction normal to the motion.
For unseparated incompressible potential flow past a two-dimensional body around which there is a circulation :
D'Alembert's Paradox:
According to D'Alembert, no energy is needed to overcome drag!
Kutta-Joukowski:
According to this, we can get nonzero lift without doing any work.
Proof of the laws: we saw before that at large distances, the velocity potential induced by the body approaches a vortex flow. So for large z:
Doing Blasius' integral along a very large circle around the body, Note that the circulation must be clockwise (increase the velocity above the airfoil) to produce upward lift.Exercise:
Approximate the airfoil as a thin flat plate 0<x<c where c is the cord length. Assume that the slip velocity above the plate is U+uu(x) and on the bottom U+ub(x) where U is the constant speed of flight. Use the Bernoulli law to find the pressures on the surface and then approximate for small uu and ub. Show that the Kutta-Joukowski value of the lift is obtained.
You should now be able to do The exercise above.