2009
DOI: 10.1088/0031-8949/80/06/065017
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Inelastic interactions and double Wronskian solutions for the Whitham–Broer–Kaup model in shallow water

Abstract: Under investigation in this paper is the Whitham–Broer–Kaup (WBK) model for the dispersive long wave in shallow water. Connection between the WBK model and a second-order Ablowitz–Kaup–Newell–Segur (AKNS) system is revealed. By means of the Darboux transformation for the second-order AKNS system, the multisoliton solutions in terms of the double Wronskian determinant for the WBK model are derived. Inelastic interactions are graphically discussed. Our results could be helpful for interpreting certain nonlinear … Show more

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Cited by 50 publications
(29 citation statements)
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“…We have also analyzed some algebraic properties of the (m +1)-component Wronskians in (16) and (17), and derived the asymptotic formulae in (26) of (21) as Z → ∓∞ for any given set of spectral parameters {λ k } N k=1 . Furthermore, we have revealed some properties for the twoand three-soliton collisions, including the asymptotic patterns of (21) with N = 2 and 3 (see Tables 1 and 2), parametric conditions in (28) and (32) for the preservation of all soliton components in the collision, phaseshift formulae in (29), (33), and (34) induced by the vector-soliton collisions, and generalized LFTs in (30), (35)- (37) for directly describing the state changes undergone by the colliding vector solitons.…”
Section: Discussionmentioning
confidence: 99%
“…We have also analyzed some algebraic properties of the (m +1)-component Wronskians in (16) and (17), and derived the asymptotic formulae in (26) of (21) as Z → ∓∞ for any given set of spectral parameters {λ k } N k=1 . Furthermore, we have revealed some properties for the twoand three-soliton collisions, including the asymptotic patterns of (21) with N = 2 and 3 (see Tables 1 and 2), parametric conditions in (28) and (32) for the preservation of all soliton components in the collision, phaseshift formulae in (29), (33), and (34) induced by the vector-soliton collisions, and generalized LFTs in (30), (35)- (37) for directly describing the state changes undergone by the colliding vector solitons.…”
Section: Discussionmentioning
confidence: 99%
“…where A and B are taken to be the real differentiable functions of x and t. Through a direct substitution to (1), we obtain the equations as follows [12]:…”
Section: Soliton Solutions Of (1)mentioning
confidence: 99%
“…Our result is novel, different from those in Refs. [6,12,13], which display the complete elastic or inelastic interactions between/among the solitons.…”
Section: Soliton Solutions Of (1)mentioning
confidence: 99%
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“…By virtue of computerized symbolic computation [23,[27][28][29][30][31][32][33][34][36][37][38][39][40][41][42][43][44][45][46], the Painlevé integrability conditions of (3) among the coefficient functions have been derived [23], which reduce all the coefficient functions to be proportional only to γ (t), giving the special Painlevé-integrable case of (3) as [23] …”
Section: Introductionmentioning
confidence: 99%