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Mixing dynamics at the confluence of two large rivers undergoing weak density variations

[PDF] Ramonetal_2014.pdf (1.184Mb)
Identificadores
URI: https://hdl.handle.net/10481/100639
DOI: 10.1002/2013JC009488
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Autor
Ramón Casañas, Cintia Luz; Armengol, Joan; Dolz, Josep; Prats, Jordi; Rueda Valdivia, Francisco José
Editorial
John Wiley & Sons
Fecha
2014
Referencia bibliográfica
Ramón, C. L., J. Armengol, J. Dolz, J. Prats, and F. J. Rueda (2014), Mixing dynamics at the confluence of two large rivers undergoing weak density variations, J. Geophys. Res. Oceans, 119, 2386–2402, doi:10.1002/2013JC009488.
Patrocinador
This work was part of a collaborative agreement between the University of Barcelona and the University of Granada to work jointly in the Project “Gestión hidráulica y técnicas de detección remota aplicada al control de poblaciones mejillón cebra: el caso del embalse de Ribarroja y el tramo inferior del río Ebro,” funded by the Spanish Ministry of the Environment.
Resumen
Simulations of tracer experiments conducted with a three-dimensional primitive-equation hydrodynamic and transport model are used to understand the processes controlling the rate of mixing between two rivers (Ebro and Segre), with distinct physical and chemical properties, at their confluence, upstream of a meandering reservoir (Ribarroja reservoir). Mixing rates downstream of the confluence are subject to hourly scale oscillations, driven partly by changes in inflow densities and also as a result of turbulent eddies that develop within the shear layer between the confluent rivers and near a dead zone located downstream of the confluence. Even though density contrasts are low—at most O(10−1) kg m−3 difference among sources—and almost negligible from a dynamic point of view—compared with inertial forces—they are important for mixing. Mixing rates between the confluent streams under weakly buoyant conditions can be of up to 40% larger than those occurring under neutrally buoyant conditions. The buoyancy effects on mixing rates are interpreted as the result of changes in the contact area available for mixing (distortion of the mixing layer). For strong density contrasts, though, when the contact area between the streams becomes nearly horizontal, larger density differences between streams will lead to weaker mixing rates, as a result of the stabilizing effect of vertical density gradients.
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