In the literature, the weir boundary condition is usually implemented imposing the weir formula at the boundaries, but this is rigorous only in subcritical steady conditions, and a more general approach is required during transients. With acceptable approximation, the non-submerged broad-crested weir behaves as a bottom step where the energy is conserved and critical conditions are attained at the top. Taking advantage of this observation, the analytic solution of the Riemann problem for the Shallow-water Equations over a dry bottom step is considered in this paper, and the momentum and mass fluxes of the analytic solution of the Riemann problem are used to impose weakly the broad-crested non-submerged weir boundary condition in a Finite Volume scheme. (C)2013 The Authors. Published by Elsevier Ltd.
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SINTEF Digital Math & Cybernet, POB 124 Blindern, NO-0314 Oslo, Norway
Norwegian Univ Sci & Technol, Dept Math, NO-7491 Trondheim, NorwaySINTEF Digital Math & Cybernet, POB 124 Blindern, NO-0314 Oslo, Norway
Holm, Havard H.
Brodtkorb, Andre R.
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SINTEF Digital Math & Cybernet, POB 124 Blindern, NO-0314 Oslo, Norway
Oslo Metropolitan Univ, Dept Comp Sci, POB 4 St Olays Plass, NO-0130 Oslo, NorwaySINTEF Digital Math & Cybernet, POB 124 Blindern, NO-0314 Oslo, Norway
Brodtkorb, Andre R.
Brostrom, Goran
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Norwegian Meteorol Inst, POB 43 Blindern, NO-0313 Oslo, Norway
Univ Gothenburg, Dept Marine Sci, POB 461, SE-40530 Gothenburg, SwedenSINTEF Digital Math & Cybernet, POB 124 Blindern, NO-0314 Oslo, Norway
Brostrom, Goran
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Christensen, Kai H.
Saetra, Martin L.
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Norwegian Meteorol Inst, POB 43 Blindern, NO-0313 Oslo, Norway
Oslo Metropolitan Univ, Dept Comp Sci, POB 4 St Olays Plass, NO-0130 Oslo, NorwaySINTEF Digital Math & Cybernet, POB 124 Blindern, NO-0314 Oslo, Norway