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An integral boundary layer model is developed in that both the Boussinesq and non-Boussinesq approximations are taken into consideration.

However, further development of the Lagrangian Boundary Layer Model is required in order to include bore-generated turbulence and to account for variable roughness and mobile beds.

A boundary layer model was assumed for the fluid mechanical behaviour of the gaseous surroundings.

In the interpretation of the experiments, a two-dimensional boundary layer model was applied successfully to model a single channel of the monolith.

Therefore, the full equation of the fluid motion is not treated, but either a boundary-layer model is applied to solve the Navier-Stokes equation or a more simplified slot-averaging model is used, in which the flow perturbation is uniform in the direction perpendicular to the main flow.

The turbulent contribution is compatible with a boundary layer model whose origin is in decaying microeddies.

The success of the zero-pressure gradient skin friction estimate is encouraging as the only modifications that need to be made to the boundary layer model to account for a bluff body are the boundary layer outer velocity distribution and the location of separation.

Comparisons among the three term asymptotic solutions, finite element (FE) results and HRR solutions are made for boundary layer model (BLM) and single edge notched (SEN) specimen.

A boundary layer kinetics model was coupled to an approach for homogeneous nucleation from supersaturated vapors and primary particle growth by condensation as well as secondary particle formation by coagulation.

In the boundary-layer model there is no need to assume that both total concentration and density are constant.

Although panel methods are generally limited to the solution of potential flow problems (i.e. inviscid, incompressible and irrotational flow), there are several boundary layer models which extend the scope of analysable problems to include those involving viscous flow.