2005
DOI: 10.1063/1.1984492
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Solitary wave dynamics in shallow water over periodic topography

Abstract: The problem of long-wave scattering by piecewise-constant periodic topography is studied both for a linear solitary-like wave pulse, and for a weakly nonlinear solitary wave [Korteweg-de Vries (KdV) soliton]. If the characteristic length of the topographic irregularities is larger than the pulse length, the solution of the scattering problem is obtained analytically for a leading wave in the framework of linear shallow-water theory. The wave decrement in the case of the small height of the topographic irregula… Show more

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Cited by 23 publications
(26 citation statements)
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“…This dynamics is known to depend on the ratio of nonlinearity length with respect to the width of the transition zone (Tappert and Zabusky, 1971;Pelinovsky, 1971;Nakoulima et al, 2005). If the solitary wave amplitude is large, the soliton quickly adapts to the local depth, so that its new length coincides with the local conditions.…”
Section: The Korteweg-de Vries Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…This dynamics is known to depend on the ratio of nonlinearity length with respect to the width of the transition zone (Tappert and Zabusky, 1971;Pelinovsky, 1971;Nakoulima et al, 2005). If the solitary wave amplitude is large, the soliton quickly adapts to the local depth, so that its new length coincides with the local conditions.…”
Section: The Korteweg-de Vries Modelmentioning
confidence: 99%
“…In this case the soliton amplitude is proportional to h −1 (x); see Ostrovsky and Pelinovsky (1970), Johnson (1973). If the solitary wave has small amplitude, and thus, large wave length, it transforms as a linear wave, and its amplitude is proportional to h −1/4 (x); see Pelinovsky (1971), Nakoulima et al (2005). As a result, the distribution of soliton amplitudes changes with depth, and the portion of largeamplitude waves enhances more significantly than the portion of smaller-amplitude solitons.…”
Section: The Korteweg-de Vries Modelmentioning
confidence: 99%
“…В результате нарушается соотношение между дисперсией и нелинейностью, характеризуемое числом Урселла [22,23]:…”
Section: трансформация солитона на уступеunclassified
“…Since the wave after the bottom step has a soliton-like shape (but it is not a soliton), the calculation of the amplitudes of the emerging solitons is relatively simple (for more details, see [22,23]) and the formula for the secondary soliton amplitudes has the following form:…”
Section: Soliton Transformation On a Bottom Stepmentioning
confidence: 99%
“…As a result, the relationship between dispersion and nonlinearity, characterized by the Ursell number [22,23]:…”
Section: Soliton Transformation On a Bottom Stepmentioning
confidence: 99%