2014
DOI: 10.1002/2013jb010841
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Traveltime delay and initial phase reversal of distant tsunamis coupled with the self‐gravitating elastic Earth

Abstract: Systematic tsunami traveltime delays of up to 15 min relative to the numerically simulated long waves from the 2010 Chilean and 2011 Tohoku-Oki earthquakes were widely observed at deep ocean tsunamimeters. Enigmatic small negative phases appearing before the main peak were commonly found only at the trans-oceanic locations. The frequency dependence of the measured tsunami phase velocities shows reverse dispersions at long periods, i.e., the tsunami speed becomes slower at periods beyond 1000 s. This is consist… Show more

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Cited by 148 publications
(153 citation statements)
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References 57 publications
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“…Both the high and the low frequency dispersion effects are expected to significantly influence the waveforms at Honolulu. Thus, all dispersion effects are introduced into the waveforms simulated by the linear long wave model based on the phase correction method developed by Watada et al (2014). In contrast, only the high frequency dispersion effect is expected to influence the waveforms of Naos Island with respect to distance relations.…”
Section: Methodsmentioning
confidence: 99%
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“…Both the high and the low frequency dispersion effects are expected to significantly influence the waveforms at Honolulu. Thus, all dispersion effects are introduced into the waveforms simulated by the linear long wave model based on the phase correction method developed by Watada et al (2014). In contrast, only the high frequency dispersion effect is expected to influence the waveforms of Naos Island with respect to distance relations.…”
Section: Methodsmentioning
confidence: 99%
“…Here, the phase correction method requires a propagation distance and average water depth during tsunami propagation. The distance was assumed to be the arc distance along the great-circle path through the subfault location and the tide gauge station, as defined by Watada et al (2014), who used a depth of 4 km as the average water depth during the propagation. However, arrival times of the waveforms simulated by the linear long wave model at the Honolulu station assumed a range of approximately 12-13 h. When the tsunami propagated following the linear long wave theory over distance and time, the equal average depth was comparable to 1.5-1.7 km with respect to the dispersion relation in the long wave condition.…”
Section: Methodsmentioning
confidence: 99%
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“…IGW phase speed c = ω/k does not exceed (gH) 1/2 and is much smaller than sound speed in water and compressional and shear wave speeds in the ocean bottom. Therefore, corrections to the dispersion equation due to water compressibility and seafloor compliance are rather small (Tsai et al 2013;Watada et al 2014) and do not change the nature of IGWs as horizontally propagating surface waves, where both k and ω are real-valued (Brekhovskikh and Godin 1998).…”
Section: Infragravity Waves and Atmospheric Wavesmentioning
confidence: 99%
“…A small reduction of the tsunami phase velocity at very long period (>1000 seconds), caused by the coupling of seawater and self-gravitating elastic Earth, is considered to be responsible for these delays [65].…”
Section: Review Of Developments In Tsunami Sciencementioning
confidence: 99%