The mechanism for the generation of vorticity at a viscous free surface is
described. This is a free-surface analogue of Lighthill's strategy for dete
rmining the vorticity flux at solid boundaries. In this method the zero-she
ar-stress and pressure boundary conditions are transformed into a boundary
integral formulation suitable for the velocity vorticity description of the
flow. A vortex sheet along the free surface is determined by the pressure
boundary condition, while the condition of zero shear stress determines the
vorticity at the surface. In general, vorticity is generated at free surfa
ces whenever there is flow past regions of surface curvature. It is shown t
hat vorticity is conserved in free-surface viscous flows. Vorticity which h
ows out of the fluid across the free surface is gained by the vortex sheet;
the integral of vorticity over the entire fluid region plus the integral o
f surface vorticity' over the free surface remains constant. The implicatio
ns of the present strategy as an algorithm for numerical calculations are d
iscussed.