Gravel threshold of motion: a state function of sediment transport disequilibrium?

In most sediment transport models, a threshold variable dictates the shear stress at which non-negligible bedload transport begins. Previous work has demonstrated that nondimensional transport thresholds (<i>τ</i><sub>c</sub>*) vary with many factors related not only to grain...

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Main Author: J. P. L. Johnson
Format: Article
Language:English
Published: Copernicus Publications 2016-08-01
Series:Earth Surface Dynamics
Online Access:http://www.earth-surf-dynam.net/4/685/2016/esurf-4-685-2016.pdf
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spelling doaj-16305f1aca6f4981bf999ee23bb747272020-11-25T01:26:00ZengCopernicus PublicationsEarth Surface Dynamics2196-63112196-632X2016-08-014368570310.5194/esurf-4-685-2016Gravel threshold of motion: a state function of sediment transport disequilibrium?J. P. L. Johnson0Department of Geological Sciences, The University of Texas, Austin, TX, USAIn most sediment transport models, a threshold variable dictates the shear stress at which non-negligible bedload transport begins. Previous work has demonstrated that nondimensional transport thresholds (<i>τ</i><sub>c</sub>*) vary with many factors related not only to grain size and shape, but also with characteristics of the local bed surface and sediment transport rate (<i>q</i><sub>s</sub>). I propose a new model in which <i>q</i><sub>s</sub>-dependent <i>τ</i><sub>c</sub>*, notated as <i>τ</i><sub>c(<i>q</i><sub>s</sub>)</sub>*, evolves as a power-law function of net erosion or deposition. In the model, net entrainment is assumed to progressively remove more mobile particles while leaving behind more stable grains, gradually increasing <i>τ</i><sub>c(<i>q</i><sub>s</sub>)</sub>* and reducing transport rates. Net deposition tends to fill in topographic lows, progressively leading to less stable distributions of surface grains, decreasing <i>τ</i><sub>c(<i>q</i><sub>s</sub>)</sub>* and increasing transport rates. Model parameters are calibrated based on laboratory flume experiments that explore transport disequilibrium. The <i>τ</i><sub>c(<i>q</i><sub>s</sub>)</sub>* equation is then incorporated into a simple morphodynamic model. The evolution of <i>τ</i><sub>c(<i>q</i><sub>s</sub>)</sub>* is a negative feedback on morphologic change, while also allowing reaches to equilibrate to sediment supply at different slopes. Finally, <i>τ</i><sub>c(<i>q</i><sub>s</sub>)</sub>* is interpreted to be an important but nonunique state variable for morphodynamics, in a manner consistent with state variables such as temperature in thermodynamics.http://www.earth-surf-dynam.net/4/685/2016/esurf-4-685-2016.pdf
collection DOAJ
language English
format Article
sources DOAJ
author J. P. L. Johnson
spellingShingle J. P. L. Johnson
Gravel threshold of motion: a state function of sediment transport disequilibrium?
Earth Surface Dynamics
author_facet J. P. L. Johnson
author_sort J. P. L. Johnson
title Gravel threshold of motion: a state function of sediment transport disequilibrium?
title_short Gravel threshold of motion: a state function of sediment transport disequilibrium?
title_full Gravel threshold of motion: a state function of sediment transport disequilibrium?
title_fullStr Gravel threshold of motion: a state function of sediment transport disequilibrium?
title_full_unstemmed Gravel threshold of motion: a state function of sediment transport disequilibrium?
title_sort gravel threshold of motion: a state function of sediment transport disequilibrium?
publisher Copernicus Publications
series Earth Surface Dynamics
issn 2196-6311
2196-632X
publishDate 2016-08-01
description In most sediment transport models, a threshold variable dictates the shear stress at which non-negligible bedload transport begins. Previous work has demonstrated that nondimensional transport thresholds (<i>τ</i><sub>c</sub>*) vary with many factors related not only to grain size and shape, but also with characteristics of the local bed surface and sediment transport rate (<i>q</i><sub>s</sub>). I propose a new model in which <i>q</i><sub>s</sub>-dependent <i>τ</i><sub>c</sub>*, notated as <i>τ</i><sub>c(<i>q</i><sub>s</sub>)</sub>*, evolves as a power-law function of net erosion or deposition. In the model, net entrainment is assumed to progressively remove more mobile particles while leaving behind more stable grains, gradually increasing <i>τ</i><sub>c(<i>q</i><sub>s</sub>)</sub>* and reducing transport rates. Net deposition tends to fill in topographic lows, progressively leading to less stable distributions of surface grains, decreasing <i>τ</i><sub>c(<i>q</i><sub>s</sub>)</sub>* and increasing transport rates. Model parameters are calibrated based on laboratory flume experiments that explore transport disequilibrium. The <i>τ</i><sub>c(<i>q</i><sub>s</sub>)</sub>* equation is then incorporated into a simple morphodynamic model. The evolution of <i>τ</i><sub>c(<i>q</i><sub>s</sub>)</sub>* is a negative feedback on morphologic change, while also allowing reaches to equilibrate to sediment supply at different slopes. Finally, <i>τ</i><sub>c(<i>q</i><sub>s</sub>)</sub>* is interpreted to be an important but nonunique state variable for morphodynamics, in a manner consistent with state variables such as temperature in thermodynamics.
url http://www.earth-surf-dynam.net/4/685/2016/esurf-4-685-2016.pdf
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