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USGS hydrologic technician Erik Ohlson measures the discharge of the Suwannee River floodwaters coming over US highway 90 near Ellaville, Florida. (Saturday, April 11, 2009)

Benthic Flux and Submarine Groundwater Discharge

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Benthic Flux and Submarine Groundwater Discharge

Calculator: Benthic flux and submarine groundwater discharge component forced by surface gravity waves on a single-unit medium of infinite thickness

This calculator solves for average benthic water discharge flux q̄bd forced by surface gravity waves on a plane bed composed of a homogeneous, isotropic porous medium of infinite thickness (Figure 1A). Submarine groundwater discharge (SGD) is qbd to a marine water body.

ParameterSymbolValueUnitKing et al. (2009) ReferenceNote
wave period T s
wave amplitude a m
gravitational acceleration g m s-2
porous medium permeability k m2
water density ρ kg m-3
water kinematic viscosity υ m2 s-1
mean water depth h m
wave frequency σ s-1 =2π/T
wave number, real component λr m-1 Equation 18
wave length L m =2π/λr
dimensionless water depth λrh
dimensionless permeability modulus R Equation 16
dimensionless model parameter P̂ Table 2
wave number, imaginary component λi m-1 Equation 19
dimensionless model parameter Q̂ Table 2
dimensionless amplitude parameter Equation 52
dimensionless amplification parameter β Equation 15
benthic flux amplitude α m s-1 Equation 14
cm d-1
average benthic water discharge flux q̄bd m s-1 Equation 55 SGD in a marine water body
cm d-1 SGD in a marine water body




 Two-dimensional, vertically oriented cross sections

Figure 1. Two-dimensional, vertically oriented cross sections, in x and z dimensions, of wave-forced benthic recharge flux qbr.w and wave-forced benthic discharge flux qbd.w, with a water surface at z = η oscillating about a still water surface at z = 0. The bed of the water body is located at z = -h;. The following domain geometry is used to solve two-dimensional boundary value problems in King et al. (2009): (A) Case I, hydrogeologic unit of infinite thickness; (B) Case II, hydrogeologic unit of finite thickness; and (C) Case III, dual-unit system, which consists of a unit of finite thickness over a unit of infinite thickness. The wave-forced velocity field transports constituents within the porous domain, over -h > z > -h - ζ



King et al. (2009) state that this model "assumes a two-dimensional x-z oriented system; linear wave; incompressible pore fluid; irrotational, inviscid flow in the surface water domain; horizontal, plane bed; rigid, homogeneous, isotropic, porous medium; laminar and viscous flow in the porous medium; case-specific, no-flow boundary conditions; Darcy's law; Equations 4 to 11 of King et al. (2009); λi<<1; R<<1; and the hydrogeologic unit concept. In a strict sense, some of these assumptions, such as a two-dimensional system, are never valid for practical applications. The abstraction process permits conclusions about the prototype to be drawn from the behavior of the model. Clearly, because Riedl et al. [1972] showed agreement between model a and observed a off Bogue Bank;" and the model "compares favorably with Yamamoto et al. [1978], it is possible to draw ... meaningful conclusions about ... natural or laboratory systems from the abstracted model."

Reference

King, J. N., A. J. Mehta, and R. G. Dean (2009), Generalized analytical model for benthic water flux forced by surface gravity waves, J. Geophys. Res., 114, C04004, doi:10.1029/2008JC005116.

Riedl, R. J., N. Huang, and R. Machan (1972), The subtidal pump: A mechanism of interstitial water exchange by wave action, Mar. Biol., 13, 210–221.

Yamamoto, T., H. L. Koning, H. Sellmeijer, and E. P. Van Hijum (1978), Response of a poro-elastic bed to water-waves, J. Fluid Mech., 87, 193–206.


Contact: jking@usgs.gov

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