Please use this identifier to cite or link to this item: http://hdl.handle.net/10773/25519
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dc.contributor.authorRuessink, B. G.pt_PT
dc.contributor.authorMichallet, H.pt_PT
dc.contributor.authorAbreu, T.pt_PT
dc.contributor.authorSancho, F.pt_PT
dc.contributor.authorVan Der A, D. A.pt_PT
dc.contributor.authorVan Der Werf, J. J.pt_PT
dc.contributor.authorSilva, P. A.pt_PT
dc.date.accessioned2019-03-08T12:05:19Z-
dc.date.available2019-03-08T12:05:19Z-
dc.date.issued2011-
dc.identifier.issn2169-9291pt_PT
dc.identifier.urihttp://hdl.handle.net/10773/25519-
dc.description.abstractU‐tube measurements of instantaneous velocities, concentrations, and fluxes for a well‐sorted, medium‐sized sand in oscillatory sheet flow are analyzed. The experiments involved two velocity‐asymmetric flows, the same two flows with an opposing current of 0.4 m/s, and a mixed skewed‐asymmetric flow, all with a velocity amplitude of 1.2 m/s and flow period of 7 s. We find that the net positive transport rate beneath velocityasymmetric oscillatory flow results from large, but opposing sand fluxes during the positive and negative flow phase. With an increase in velocity asymmetry and, in particular, velocity skewness, the difference in the magnitude of the fluxes in the two half cycles increases, leading to larger net transport rates. This trend is consistent with the observed increase in skewness of the oscillatory bed shear stress. Phase‐lag effects, whereby sand stirred during the negative flow phase has not settled by the time of the negative‐to‐positive flow reversal and is subsequently transported during the positive flow phase, are notable but of minor importance to the net transport rate compared to earlier experiments with finer sands. In the vertical, the oscillatory flux is positive above the noflow bed. Within the sheet flow pick‐up layer, the oscillatory flux is negative and similar in magnitude to the positive flux induced by the residual flow. The 0.4 m/s opposing current causes more sand to be picked up during the negative than during the positive flow phase. Above the no‐flow bed the resulting negative oscillatory flux is comparable in magnitude to the current‐related flux.pt_PT
dc.description.sponsorshipThe work presented here was part of the TRANSKEW project supported by the European Community’s Sixth Framework Programme through the grant to the budget of the Integrated Infrastructure Initiative HYDRALAB III, contract 022441 (RII3). B.G.R. acknowledges additional funding by the Netherlands Organisation for Scientific Research NWO under project 864.04.007. We thank André Temperville, Tom O’Donoghue, Jan Ribberink, Paula Freire, Sandra Plecha, Kate Steenhauer, Gustaaf Kikkert, John Cornelisse, and Noureddine Ait Lafkih for their help and technical support during the experiments. Supported by the HYDRALAB III project SANDS, Maarten Kleinhans assisted with the inversion of the ABS voltage to sand concentration and David Hurther developed the hardware and software used to process the ADVP data. Useful and constructive comments from three anonymous reviewers helped improve the manuscript.pt_PT
dc.language.isoengpt_PT
dc.publisherAmerican Geophysical Unionpt_PT
dc.rightsopenAccesspt_PT
dc.titleObservations of velocities, sand concentrations, and fluxes under velocity-asymmetric oscillatory flowspt_PT
dc.typearticlept_PT
dc.description.versionpublishedpt_PT
dc.peerreviewedyespt_PT
degois.publication.firstPage1 - C03004pt_PT
degois.publication.lastPage13 - C03004pt_PT
degois.publication.titleJournal of Geophysical Research: Oceanspt_PT
degois.publication.volume116pt_PT
dc.identifier.doi10.1029/2010JC006443pt_PT
dc.identifier.essn2169-9291pt_PT
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