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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