2009
DOI: 10.1029/2008gl037030
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Observation of swell dissipation across oceans

Abstract: [1] Global observations of ocean swell, from satellite Synthetic Aperture Radar data, are used to estimate the dissipation of swell energy for a number of storms. Swells can be very persistent with energy e-folding scales exceeding 20,000 km. For increasing swell steepness this scale shrinks systematically, down to 2800 km for the steepest observed swells, revealing a significant loss of swell energy. This value corresponds to a normalized energy decay in time b = 4.2 Â 10 À6 s À1 . Many processes may be respo… Show more

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Cited by 286 publications
(294 citation statements)
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“…Waves that propagate away from their generation area and no longer receive energy input from the local wind are called swell. Swell waves can travel long distances across the ocean, up to 20,000 km, half of the Earth's perimeter [1][2][3][4]. Since swells can propagate such long distances, the wave field is, most of the times, the result of contributions from waves with different frequencies (periods) and incoming directions: wind seas, and young and old swell waves, reflecting different origins and ages.…”
Section: Introductionmentioning
confidence: 99%
“…Waves that propagate away from their generation area and no longer receive energy input from the local wind are called swell. Swell waves can travel long distances across the ocean, up to 20,000 km, half of the Earth's perimeter [1][2][3][4]. Since swells can propagate such long distances, the wave field is, most of the times, the result of contributions from waves with different frequencies (periods) and incoming directions: wind seas, and young and old swell waves, reflecting different origins and ages.…”
Section: Introductionmentioning
confidence: 99%
“…Young and Babanin (2006) arrived at a similar conclusion and also proposed a cumulative source term. Observations of swell dissipation over long distances resulted in a separate dissipation term for swell associated with turbulence (Ardhuin et al 2009) in the upper layer of the ocean. Significant progress was made by Ardhuin et al (2010) who combined the effects of local saturation (but scaled with the absolute excess of wave variance), cumulative effects and a separate swell dissipation term.…”
Section: Introductionmentioning
confidence: 99%
“…(7), β capil is the damping term of capillary waves due to the viscosity of water, and is taken from Lamb (1932) as β capil = −4 ν w k 2 , where ν w = 1.3 × 10 −6 m 2 s −1 is the kinematic viscosity of water. According to Dore (1978), however, the viscosity of the air gives a stronger dissipation for wavelength larger than 0.85 m. Swell dissipation was observed by Tolman (2002) and Ardhuin et al (2009), who found it to be consistent with the effects of friction with the atmosphere. The term β swell in Eq.…”
Section: Viscous Damping Termmentioning
confidence: 57%
“…where c g is wave group velocity, (∂F /∂t) w represents the wind input term, (∂F /∂t) visc accounts for the damping of capillary waves due to water viscosity, and also includes a swell dissipation term related to friction with the atmosphere, as reported by several studies (Tolman, 2002;Ardhuin et al, 2009), as will be discussed below. The other terms of the right-hand side of Eq.…”
Section: Spectral Evolution Equations Integrated Over Wavenumbermentioning
confidence: 99%