Abstract
(7) with r — ^/(x2 + z2) the distance from the symmetry axis. These results can now be used for the calculation of the viscous effect on the stagnation pressure for, respectively, a circular cylinder and a sphere placed in a parallel flow, for the limit of large Reynolds number.5 In that case the viscous layer thickness is small with respect to the body radius, and the local stagnation area can be approximated with the corresponding stagnation flow. Taking the inviscid outer flow distribution from potential theory, we find Cylinder:
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