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Sediment deposition from turbidity currents in simulated aquatic vegetation canopies
Author(s) -
Soler Marianna,
Colomer Jordi,
Serra Teresa,
Casamitjana Xavier,
Folkard Andrew M.
Publication year - 2017
Publication title -
sedimentology
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.494
H-Index - 108
eISSN - 1365-3091
pISSN - 0037-0746
DOI - 10.1111/sed.12342
Subject(s) - flume , turbidity current , geology , current (fluid) , sediment , drag coefficient , drag , deposition (geology) , flux (metallurgy) , hydrology (agriculture) , sedimentary rock , geomorphology , geotechnical engineering , flow (mathematics) , sedimentary depositional environment , oceanography , geometry , mechanics , materials science , physics , structural basin , paleontology , mathematics , metallurgy
Abstract A laboratory flume experiment was carried out in which the hydrodynamic and sedimentary behaviour of a turbidity current was measured as it passed through an array of vertical rigid cylinders. The cylinders were intended primarily to simulate aquatic vegetation canopies, but could equally be taken to represent other arrays of obstacles, for example forests or offshore wind turbines. The turbidity currents were generated by mixing naturally sourced, poly‐disperse sediment into a reservoir of water at concentrations from 1·0 to 10·0 g l −1 , which was then released into the experimental section of the flume by removing a lock gate. For each initial sediment concentration, runs with obstacle arrays with solid plant fractions of 1·0% and 2·5%, and control cases with no obstacles, were carried out. The progress of the current along the flume was characterized by the array drag term, C D ax c (where C D is the array drag coefficient, at the frontal area of cylinders per unit volume, and x c is the position of the leading edge of the current along the flume). The downward depositional flux of sediment out of the current as it proceeded was measured at 13 traps along the flume. Analysis of these deposits divided them into fine (2·2 to 6·2 μm) and coarse (6·2 to 104 μm) fractions. At the beginning of their development, the gravity currents proceeded in an inertia‐dominated regime until C D ax c = 5. For C D ax c > 5, the current transitioned into a drag‐dominated regime. For both fine and coarse sediment fractions, the rate of sediment deposition tended to decrease gradually with distance from the source in the inertial regime, remained approximately constant at the early drag‐dominated regime, and then rose and peaked at the end of the drag‐dominated stage. This implies that, when passing through arrays of obstacles, the turbidity currents were able to retain sufficient sediment in suspension to maintain their flow until they became significantly influenced by the drag exerted by the obstacles.