Please use this identifier to cite or link to this item: http://repositorio.lnec.pt:8080/jspui/handle/123456789/1002460
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dc.contributor.authorRuessink, B. G.pt_BR
dc.contributor.authorMichallet, H.pt_BR
dc.contributor.authorAbreu, T.pt_BR
dc.contributor.authorSancho, F. E.pt_BR
dc.contributor.authorVan der A, D. A.pt_BR
dc.contributor.authorVan der Werf, J. J.pt_BR
dc.contributor.authorSilva, P. A.pt_BR
dc.date.accessioned2011-09-02T16:00:31Zpt_BR
dc.date.accessioned2014-10-20T09:50:41Zpt_BR
dc.date.accessioned2016-04-28T14:14:41Z-
dc.date.available2011-09-02T16:00:31Zpt_BR
dc.date.available2014-10-20T09:50:41Zpt_BR
dc.date.available2016-04-28T14:14:41Z-
dc.date.issued2011-03pt_BR
dc.identifier.urihttps://repositorio.lnec.pt/jspui/handle/123456789/1002460-
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_BR
dc.language.isoengpt_BR
dc.rightsrestrictedAccesspt_BR
dc.titleObservations of velocities, sand concentrations, and fluxes under velocity‐asymmetric oscillatory flowspt_BR
dc.typeworkingPaperpt_BR
dc.description.figures8pt_BR
dc.description.tables2pt_BR
dc.description.pages13 ppt_BR
dc.description.volumeVOL. 116pt_BR
dc.description.sectorDHA/NECpt_BR
dc.description.magazineJOURNAL OF GEOPHYSICAL RESEARCHpt_BR
Appears in Collections:DHA/NEC - Comunicações a congressos e artigos de revista

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