Abstract
The unsteady, axially symmetric stagnation-point flow problem for an incompressible fluid past a body of revolution, with velocity outside the boundary layer fluctuating with time as U0(x){1+εeiwt} is investigated. By assuming U0(x)=u1x+u3x3+···, and using Howarth’s corresponding power series solution for steady flow, a power series for the fluctuating velocity component is obtained, the coefficients of which are universal functions of η=y(2u1⁄ν)1⁄2, with ω as a parameter. Numerical calculations performed show that the variation of skin friction from the steady-state value becomes insignificant as the point of separation is approached.