Undular and broken surges in dam-break flows: a review of wave breaking strategies in a Boussinesq-type framework

The water waves resulting from the collapse of a dam are important unsteady free surface flows in civil and environmental engineering. Considering the basic case of ideal dam break waves in a horizontal and rectangular channel the wave patterns observed experimentally depends on the initial depths d...

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Veröffentlicht in:Environmental fluid mechanics (Dordrecht, Netherlands : 2001) Netherlands : 2001), 2020-12, Vol.20 (6), p.1383-1416
Hauptverfasser: Castro-Orgaz, Oscar, Chanson, Hubert
Format: Artikel
Sprache:eng
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Zusammenfassung:The water waves resulting from the collapse of a dam are important unsteady free surface flows in civil and environmental engineering. Considering the basic case of ideal dam break waves in a horizontal and rectangular channel the wave patterns observed experimentally depends on the initial depths downstream ( h d ) and upstream ( h o ) of the dam. For r  =  h d / h o above the transition domain 0.4–0.55, the surge travelling downstream is undular, a feature described by the dispersive Serre–Green–Naghdi (SGN) equations. In contrast, for r below this transition domain, the surge is broken and it is well described by the weak solution of the Saint–Venant equations, called Shallow Water Equations (SWE). Hybrid models combining SGN–SWE equations are thus used in practice, typically implementing wave breaking modules resorting to several criteria to define the onset of breaking, frequently involving case-dependent calibration of parameters. In this work, a new set of higher-order depth-averaged non-hydrostatic equations is presented. The equations consist in the SGN equations plus additional higher-order contributions originating from the variation with elevation of the velocity profile, modeled here with a Picard iteration of the potential flow equations. It is demonstrated that the higher-order terms confer wave breaking ability to the model without using any empirical parameter, such while, for r  > 0.4–0.55, the model results are essentially identical to the SGN equations but, for r  
ISSN:1567-7419
1573-1510
DOI:10.1007/s10652-020-09749-3