ABSTRACT
Consider the stationary Prandtl system for a planar incompressible flow () v ∂ 2 u ∂ y 2 − u ∂ u ∂ x − υ ∂ u ∂ y = − U ( x ) d U ( x ) d x , ∂ u ∂ x + ∂ υ ∂ y = 0 , https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9780203749364/8d969161-112a-446e-ae5c-4c9e50da0b93/content/eq3784.tif"/>
