Generation of dense plume fingers in saturated-unsaturated homogeneous porous media

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Authors

  • Clemens J.M. Cremer
  • Thomas Graf
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Details

Original languageEnglish
Pages (from-to)69-82
Number of pages14
JournalJournal of contaminant hydrology
Volume173
Early online date8 Dec 2014
Publication statusPublished - Feb 2015

Abstract

Flow under variable-density conditions is widespread, occurring in geothermal reservoirs, at waste disposal sites or due to saltwater intrusion. The migration of dense plumes typically results in the formation of vertical plume fingers which are known to be triggered by material heterogeneity or by variations in source concentration that causes the density variation. Using a numerical groundwater model, six perturbation methods are tested under saturated and unsaturated flow conditions to mimic heterogeneity and concentration variations on the pore scale in order to realistically generate dense fingers. A laboratory-scale sand tank experiment is numerically simulated, and the perturbation methods are evaluated by comparing plume fingers obtained from the laboratory experiment with numerically simulated fingers. Dense plume fingering for saturated flow can best be reproduced with a spatially random, time-constant perturbation of the solute source. For unsaturated flow, a spatially and temporally random noise of solute concentration or a random conductivity field adequately simulate plume fingering.

Keywords

    Density, Fingering, Groundwater, Model, Numerical trigger, Saturated, Unsaturated

ASJC Scopus subject areas

Cite this

Generation of dense plume fingers in saturated-unsaturated homogeneous porous media. / Cremer, Clemens J.M.; Graf, Thomas.
In: Journal of contaminant hydrology, Vol. 173, 02.2015, p. 69-82.

Research output: Contribution to journalArticleResearchpeer review

Cremer CJM, Graf T. Generation of dense plume fingers in saturated-unsaturated homogeneous porous media. Journal of contaminant hydrology. 2015 Feb;173:69-82. Epub 2014 Dec 8. doi: 10.1016/j.jconhyd.2014.11.008
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