1980
DOI: 10.1175/1520-0485(1980)010<0605:ioowwa>2.0.co;2
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Interaction of Ocean Waves with a Soft Bottom

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Cited by 83 publications
(31 citation statements)
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“…Viscosity of (un-reconstituted) muds is not known with any certainty, but it has been measured on a few samples by Jiang and Mehta (1995) and Hsiao and Shemdin (1980). The range is large, from 225 to 140,000 Pa s, and when placed in the Algar et al (2011a) rise model, speeds of 0.2e47 cm s À1 result.…”
Section: Initial Bubble Risementioning
confidence: 99%
“…Viscosity of (un-reconstituted) muds is not known with any certainty, but it has been measured on a few samples by Jiang and Mehta (1995) and Hsiao and Shemdin (1980). The range is large, from 225 to 140,000 Pa s, and when placed in the Algar et al (2011a) rise model, speeds of 0.2e47 cm s À1 result.…”
Section: Initial Bubble Risementioning
confidence: 99%
“…The imaginary part of k then gives the rate of spatial attenuation. Mud has also been modelled as a Kelvin-Voigt viscoelastic body by MacPherson (1980), Hsiao & Shemdin (1980) and Maa & Mehta (1988), where the coefficients of viscosity and elasticity are assumed to be constants. Second-order theories on the mass transport in fluid mud have been reported by Shibayama, Okuno & Sato (1990), Foda, Hunt & Chou (1993) and Piedra-Cueva.…”
Section: Introductionmentioning
confidence: 99%
“…The dissipation rate of waves propagating over mud bottoms is considerably higher than over sandy bottoms. For a more detailed description see, e.g., Dean and Dalrymple (1984), Gade (1958), Hsiao and Shemdin (1980), and Cavaleri p.169 in (Komen et al, 1994). Winterwerp et al (2005) give a formulation for the energy dissipation source term which they used in the SWAN model.…”
Section: Energy Dissipation Due To Wave-bottom Interactionmentioning
confidence: 99%