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Equation () can be solved explicitly for
the depth field at the arrival point in terms of the divergence of the velocity field as
where
Further, () can be simplified to express in terms of as follows,
where
If we then insert () into () and assume as known,
then we have a linear elliptic equation for ,
where the right-hand-side is known and is the linear elliptic
operator such that
Equations () and () constitute our
implicit free surface semi-Lagrangian
shallow water model formulated in terms of an elliptic equation for the velocity
field.
Balasubramany (Balu) Nadiga
1/8/1998