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Bursts in discontinuous Aeolian saltation

Close to the onset of Aeolian particle transport through saltation we find in wind tunnel experiments a regime of discontinuous flux characterized by bursts of activity. Scaling laws are observed in the time delay between each burst and in the measurements of the wind fluctuations at the fluid thres...

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Autores principales: Carneiro, M. V., Rasmussen, K. R., Herrmann, H. J.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2015
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4466891/
https://www.ncbi.nlm.nih.gov/pubmed/26073305
http://dx.doi.org/10.1038/srep11109
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author Carneiro, M. V.
Rasmussen, K. R.
Herrmann, H. J.
author_facet Carneiro, M. V.
Rasmussen, K. R.
Herrmann, H. J.
author_sort Carneiro, M. V.
collection PubMed
description Close to the onset of Aeolian particle transport through saltation we find in wind tunnel experiments a regime of discontinuous flux characterized by bursts of activity. Scaling laws are observed in the time delay between each burst and in the measurements of the wind fluctuations at the fluid threshold Shields number θ(c). The time delay between each burst decreases on average with the increase of the Shields number until sand flux becomes continuous. A numerical model for saltation including the wind-entrainment from the turbulent fluctuations can reproduce these observations and gives insight about their origin. We present here also for the first time measurements showing that with feeding it becomes possible to sustain discontinuous flux even below the fluid threshold.
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spelling pubmed-44668912015-06-18 Bursts in discontinuous Aeolian saltation Carneiro, M. V. Rasmussen, K. R. Herrmann, H. J. Sci Rep Article Close to the onset of Aeolian particle transport through saltation we find in wind tunnel experiments a regime of discontinuous flux characterized by bursts of activity. Scaling laws are observed in the time delay between each burst and in the measurements of the wind fluctuations at the fluid threshold Shields number θ(c). The time delay between each burst decreases on average with the increase of the Shields number until sand flux becomes continuous. A numerical model for saltation including the wind-entrainment from the turbulent fluctuations can reproduce these observations and gives insight about their origin. We present here also for the first time measurements showing that with feeding it becomes possible to sustain discontinuous flux even below the fluid threshold. Nature Publishing Group 2015-06-15 /pmc/articles/PMC4466891/ /pubmed/26073305 http://dx.doi.org/10.1038/srep11109 Text en Copyright © 2015, Macmillan Publishers Limited http://creativecommons.org/licenses/by/4.0/ This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/
spellingShingle Article
Carneiro, M. V.
Rasmussen, K. R.
Herrmann, H. J.
Bursts in discontinuous Aeolian saltation
title Bursts in discontinuous Aeolian saltation
title_full Bursts in discontinuous Aeolian saltation
title_fullStr Bursts in discontinuous Aeolian saltation
title_full_unstemmed Bursts in discontinuous Aeolian saltation
title_short Bursts in discontinuous Aeolian saltation
title_sort bursts in discontinuous aeolian saltation
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4466891/
https://www.ncbi.nlm.nih.gov/pubmed/26073305
http://dx.doi.org/10.1038/srep11109
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