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The boundary layer technique is encountered in many aspects of fluid dynamics and aerodynamics.

The viscous region is modeled using a finite difference boundary layer technique.

We extend to the variable coefficient case boundary layer techniques that have been successful in the treatment of the Laplace equation and certain other constant coefficient elliptic partial differential equations on Lipschitz domains in Euclidean space.

Otherwise, the PHY layer techniques are irrelevant.

This approximate boundary integral technique is based upon the integral representation for scattered elastic waves using single-layer boundary sources.

The boundary layer saturation is Eq. 18.

Boundary layer transition is caused by small disturbances within the boundary layer that grow via a variety of mechanisms to cause turbulence.

To improve the subdivided-volume simulation of convection-related parameters, a modeling technique (boundary layer flow approximation) was devised.

Three boundary layer problems are considered and solved in this study using the novel technique.

The top of the daytime boundary layer is referred to as the mixed-layer inversion.

This boundary layer is approximately 0.3 nm thick.