Water wave-driven seepage in marine sediments
Introduction
Sediments in bays, estuaries, and in the seabed near river inlets are often contaminated. Many inorganic contaminants (notably heavy metals) do not decompose. Under certain conditions, these accumulated substances can be released back into the receiving body of water through mass transfer processes at the seabed. The mass transfer rate is largely controlled by the seepage flux exchange between the sediment and the seawater [26]. Increased wave action and higher sediment hydraulic conductivity generally cause larger transfer rates. Clearly, quantification of the mass transfer rate is a key factor in water quality modelling.
Water wave effects on the marine sediment in shallow water have been studied intensively in the last few decades. Most earlier studies [1], [18], [19], [21], [23] were based on the assumption that the porous seabed was non-deformable, and that the pore water was incompressible. Numerous investigations have been carried out based on Biot's consolidation equation [2] and the assumptions of a compressible pore fluid and soil skeleton. The seabed has been modelled as being isotropic [9], [20], [22], [29], [30], anisotropic [10] and inhomogeneous [16]. The potential for extreme seabed instability (such as liquefaction) due to a generalised three-dimensional wave system has recently been explored [17]. Limitations and applications of previous investigations have been reviewed also [11]. Two major shortcomings of most previous approximations in the area of wave–seabed interaction are:
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Assumption of a quasi-static state: The dynamic terms generated from the acceleration of soil particles and the movement of pore fluid were not included in most previous solutions. Although the inertia effect generated from the acceleration of soil particles was recently considered in the wave–seabed interaction problem [15], the acceleration due to pore fluid was excluded from the analysis. Thus, it is not a complete dynamic solution.
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Wave pressures at the seabed surface obtained from conventional ocean wave theories: These wave pressures were based on the assumption of an impermeable seabed. However, the wave pressures were then applied to a porous seabed. This contradiction has been removed recently [12], with the assumption of a quasi-static state, not a dynamic state. Recently, Liu and Wen [19] derived a fully non-linear, diffusion and weakly dispersive wave equation for describing gravity surface wave propagation in a shallow porous medium. However, they only considered a rigid medium (such as rock). Thus, only soil permeability is included in their dispersion relation.
The objective of this paper is to overcome these two shortcomings and investigate water wave-driven seepage flux into and out of the seabed under more realistic conditions. Based on the governing equations presented by Mei [22], which were derived on the basis of poro-elastic theory [3], a closed-form analytical solution for dynamic wave–seabed interactions is derived. The model also includes a new wave–dispersion relation, which accounts for the characteristics (including soil permeability, shear modulus, porosity, etc.). A comparison of the present dynamic and previous quasi-static solution is performed. Then, the effects of wave and seabed characteristics on the seepage flux at the seabed surface are investigated in a parametric study.
Section snippets
Boundary value problem
In this study, we consider a gravity wave propagating over a porous seabed. The wave crests are assumed to propagate in the positive x-direction, while the z-direction is upward from the seabed surface, as shown in Fig. 1.
The proposed model for wave–seabed interaction is based on combining incompressible irrotational flow for the water waves and Biot's poro-elastic theory [3] for flow within the porous soil skeleton.
Closed-form solution for porous flow
From , , , the velocity potential can be expressed as [6]Note that the wave number λ is an unknown parameter here. Then, the wave pressure, pw, can be written as [6]In general, the mechanism of the wave-induced seabed response can be classified into two categories, depending upon how the pore water pressure is generated [25]. One is caused by the residual or progressive nature of the excess pore pressure, which
Wave-driven seepage
Water wave over a porous seabed drives a seepage flux into and out of the sediment. As noted above, the volume of fluid exchanged per wave cycle directly relates to the mass transport rate of contaminants in the sediment, an important quantity in water quality modelling.
The net seepage flux over one wave cycle is zero. However, for the mass transport caused by the cyclic wave motion, the relevant quantity is the volume of water pumped into over one-half wave period (T) and one-half wavelength (L
Conclusions
In this paper, we derive a closed-form analytical solution of dynamic flow in a porous seabed coupling the wave motion and porous medium flow. Based on the solution, the wave-driven seepage flux into and out of the marine sediment was investigated. From the numerical examples presented, the following points can be made:
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A comparison of the wave-induced soil response between dynamic and quasi-static solutions demonstrates that pore fluid and soil skeleton accelerations can significantly increase
Acknowledgements
The authors are grateful for the valuable comments from the reviewers.
References (31)
- et al.
On calculating the lengths of water waves
Coastal Eng
(1990) On calculating the length of a short-crested wave over a porous seabed
Appl Ocean Res
(2000)- et al.
Wave-induced seabed instability: difference between liquefaction and shear failure
Soils Found
(1998) - Badiey M, Jaya I, Magda W, Ricinine W. Analytical and experimental approach in modeling of water–seabed interaction....
General theory of three-dimensional consolidation
J Appl Phys
(1941)Theory of propagation of elastic waves in a fluid–saturated porous solid, I. Low frequency range
J Acoust Soc Amer
(1956)- et al.
Consolidation of a cross-anisotropic soil medium
Q J Mech Appl Math
(1984) - Chen WF, Saleeb AF. Constitutive equations for engineering materials vol. 1. New York: Wiley;...
- et al.
Water wave mechanics for engineers and scientists
(1984) - et al.
Implication of gas content for predicting the stability of submarine slopes
Mar Geotechnol
(1977)
Wave-induced soil instability in an unsaturated anisotropic seabed of finite thickness
Int J Numer Anal Meth Geomech
Soil response in cross-anisotropic seabed due to standing waves
J Geotechnol Geoenviron Encount ASCE
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