Leading linear growth rates for steady uniform morphodynamic overland flows at different Froude numbers and grain diameters (NERC Grant NE/S00274X/1)
Shallow overland flows in steady state can become unstable and break up into destructive surges. The following data documents maximum growth rates for disturbances to uniform steady flows on a fixed slope in a one-dimensional shallow-layer model that incorporates the mechanics of erosion and deposition of monodisperse sediment, documented in sections 2 and 4 of the following freely available preprint: https://arxiv.org/abs/2007.15989. The data comprises the following 4 columns, separated by spaces: grain diameter, Froude number, solid fraction and maximum growth rate. Grain diameter refers to the characteristic diameter of erodible particles, non-dimensionalised by the steady flow depth h0. Froude number, Fr, is a dimensionless constant defined as Fr = u0 / sqrt(h0 * g'), where u0 is the velocity of the steady flow and g' is gravitational acceleration resolved perpendicular to the slope. Solid fraction is a number between 0 and 1 that describes the proportion of solid particles in the flowing mixture. A solid fraction of 0 denotes a purely fluid flow and a solid fraction of 1 denotes a saturated mixture containing a maximum packing of solid particles. Maximum growth rate refers to the largest linear growth rate for perturbations to a uniform flowing layer with the corresponding properties given in the prior 3 columns. The model formulation describes the dynamics of 4 unknown observables: flow height, flow velocity, solids concentration and bed height. By taking the 'maximum' in this case, we mean the maximum over these 4 flow fields that may be perturbed by an environmental disturbance and also the maximum over all possible wavelengths of disturbance. We note that in this dataset, flows with a maximum growth rate equal to zero or small positive values (e.g. up to machine precision) are stable; flows with strictly positive growth rate are unstable. Zero growth rate indicates that the maximum growth rate is given by a neutrally stable perturbation and such perturbations always exist for reasons of symmetry in the model. For each grain diameter and Froude number in the dataset, there exist two steady uniform states with different solid fractions. Therefore two files are supplied - one containing data for the more dilute states and the other containing data for the more concentrated states. These various technical details, as well as full documentation of the model and the parameters used are explained more fully in the aforementioned paper.
nonGeographicDataset
https://webapps.bgs.ac.uk/services/ngdc/accessions/index.html#item139765
name: Data
function: download
http://data.bgs.ac.uk/id/dataHolding/13607693
eng
geoscientificInformation
publication
2008-06-01
NGDC Deposited Data
Fluid dynamics
revision
2022
NERC_DDC
2020-12-01
2020-12-01
creation
2020-12-01
notApplicable
The data was generated by numerical solution of the linear stability problem detailed in https://arxiv.org/abs/2007.15989. For each given grain diameter and Froude numbers in the dataset, the solid fraction for a steady state is computed using a numerical root-finding algorithm. Then using a numerical eigenvalue solver available in the Julia programming language, linear growth rates are obtained for (nondimensionalised) disturbance wavenumbers between 0 and 10^6. The maximum, or leading growth rate is then the maximum over the set of wavenumbers and the four linear stability modes.
publication
2011
false
See the referenced specification
publication
2010-12-08
false
See http://eur-lex.europa.eu/LexUriServ/LexUriServ.do?uri=OJ:L:2010:323:0011:0102:EN:PDF
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Earth Sciences
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School of Mathematics
University of Bristol
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British Geological Survey
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British Geological Survey
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