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:
![]()
![]()