
High‐resolution numerical modeling of wave‐supported gravity‐driven mudflows
Author(s) -
Hsu TianJian,
Ozdemir Celalettin E.,
Traykovski Peter A.
Publication year - 2009
Publication title -
journal of geophysical research: oceans
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.67
H-Index - 298
eISSN - 2156-2202
pISSN - 0148-0227
DOI - 10.1029/2008jc005006
Subject(s) - mudflow , geology , rheology , mechanics , drag , drag coefficient , sediment transport , geotechnical engineering , sediment , geomorphology , physics , thermodynamics , landslide
Wave‐supported gravity‐driven mudflow has been identified as a major offshore fine sediment transport mechanism of terrestrial sediment into the coastal ocean. This transport process essentially occurs within the wave boundary layer. In this study, wave‐supported gravity‐driven mudflow is investigated via a wave‐phase‐resolving high‐resolution numerical model for fluid mud transport. The model results are verified with field observation of sediment concentration and near‐bed flow velocities at Po prodelta. The characteristics of wave‐supported gravity‐driven mudflows are diagnosed by varying the bed erodibility, floc properties (fractal dimension), and rheological stresses in the numerical simulations. Model results for moderate concentration suggest that using an appropriately specified fractal dimension, the dynamics of wave‐supported gravity‐driven mudflow can be predicted without explicitly incorporating rheological stress. However, incorporating rheological stress makes the results less sensitive to prescribed fractal dimension. For high‐concentration conditions, it is necessary to incorporate rheological stress in order to match observed intensity of downslope gravity‐driven current. Model results are further analyzed to evaluate and calibrate simple parameterizations. Analysis suggests that when neglecting rheological stress, the drag coefficient decreases with increasing wave intensity and seems to follow a power law. However, when rheological stress is incorporated, the resulting drag coefficient is more or less constant (around 0.0013) for different wave intensities. Model results further suggest the bulk Richardson number has a magnitude smaller than 0.25 and is essentially determined by the amount of available soft mud (i.e., the erodibility), suggesting a supply limited condition for unconsolidated mud.