2021
DOI: 10.1016/j.apor.2021.102816
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An analytical model for mass transport calculations in a viscous muddy layer

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Cited by 1 publication
(2 citation statements)
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“…We consider first the flow region before the surface obstacle, i.e., Region 1: x < −B. To satisfy the Laplace Equation (23), by the method of eigenfunction expansions, the solution form for Φ is formulated as…”
Section: Water Layermentioning
confidence: 99%
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“…We consider first the flow region before the surface obstacle, i.e., Region 1: x < −B. To satisfy the Laplace Equation (23), by the method of eigenfunction expansions, the solution form for Φ is formulated as…”
Section: Water Layermentioning
confidence: 99%
“…Due to the diverse rheological properties of fluid mud partly as a consequence of its distinct physico-chemical compositions, it is unequivocal that no single model is capable of describing the entire spectrum of rheological behaviors of fluid mud. Recent analytical results for wave-mud interactions include a depth-integrated model for weakly nonlinear long waves over a thin layer of viscoelastic mud on a mild-slope beach [21], a Boussinesq-type model incorporating two distinct soft mud layers to take into account the vertical variation of mud properties [22], and a linear theory for waves and currents over a viscoud fluid bed [23].…”
Section: Introductionmentioning
confidence: 99%