Abstract
The exact kinematic bottom boundary condition is w = u·∇h. The linearized form in an incompressible flow is w = ∇·(uh at z = 0. Use of the approximate linearized form w = u·∇h at z = 0 eliminates the phase shift of the transmitted wave in a Kelvin wave scattering calculation, and it significantly modifies the transmitted and reflected waves in a one-dimensional long-wave scattering calculation, even when u·∇hh∇·u over most of the topography.

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