1957
DOI: 10.1029/tr038i005p00662
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On the damping of gravity waves over a permeable sea bed

Abstract: The problem of damping of gravity waves over a permeable sea bed of great depth is re‐examined, using a more rigorous approach than that employed by Putnam in 1949 It is found that Putnam's approximate method of analysis is justified in view of the smallness of the permeability factors commonly encountered. However, a misinterpretation error was discovered in Putnam's paper which makes his dissipation function too great by a factor of four

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Cited by 132 publications
(68 citation statements)
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“…(16) reduces to the wave damping rate of Reid and Kajiura(1957) for an infinitely deep permeable bed.…”
Section: Damping Of Water Waves Over Permeable Bed Of Finite Depthmentioning
confidence: 99%
See 1 more Smart Citation
“…(16) reduces to the wave damping rate of Reid and Kajiura(1957) for an infinitely deep permeable bed.…”
Section: Damping Of Water Waves Over Permeable Bed Of Finite Depthmentioning
confidence: 99%
“…Reid and Kajiura(1957) derived the damping rate of waves traveling over an infinitely deep permeable seabed on the assumption that the flow inside the bed is governed by the Darcy's equation. Later, Liu and Dalrymple(1984) derived the wave damping rate over a permeable seabed of finite depth by expressing the flow inside the bed by the generalized Darcy's equation, which considers additional wave damping inside the boundary layers between water and soil and between soil and impermeable stratum.…”
Section: Introductionmentioning
confidence: 99%
“…2 It will be convenient to define a modification factor K , which includes the above considerations, and which naturally will vary with wave period, water depth, bottom conditions, etc. , such that the wave spectrum in shallow water becomes JVC*) ^vr'JV ct) y ^ J ... (12) or in terms of frequency xyt*) »***>*(>0 (13) If the continental shelf is steep, such as off the Pacific Coast of the United States, wave energy loss due to bottom friction and percolation will be negligible. If the wave crests are parallel to parallel bottom contours, refraction will be absent, and if no waves break, then the modification will be due entirely to shoaling, whence K = K .…”
Section: {11)mentioning
confidence: 99%
“…Based on the assumption of a rigid and permeable sandy seabed, Reid and Kajiura (1957) may be the first to investigate the phenomenon of wave damping analytically. Later, this method has been further extended to more complicated cases (Liu, 1973;Dean and Dalrymple, 1984;Kim et al, 2000).…”
Section: Introductionmentioning
confidence: 99%