Solitons and rouge waves for a generalized (3+1)-dimensional variable-coefficient Kadomtsev–Petviashvili equation in fluid mechanics. (May 2016)

• Record Type: Journal Article
• Authors: Chai, Jun; Tian, Bo; Sun, Wen-Rong; Xie, Xi-Yang
• Is Part Of: Computers & mathematics with applications. Volume 71:issue 10(2016)
• Page Start: 2060
• Page End: 2068
• Publication Date: 2016-05
• Subjects: Fluid mechanics -- Generalized (3+1)-dimensional variable-coefficient Kadomtsev–Petviashvili equation -- Auto-Bäcklund transformation -- Solitons -- Rouge waves -- Homoclinic breather waves; Electronic data processing -- Periodicals; Mathematics -- Data processing -- Periodicals; 510.28541
• DOI: 10.1016/j.camwa.2016.03.022
• Languages: English
• ISSNs: 0898-1221

Abstract

Abstract: Evolution of the long water waves and small-amplitude surface waves with the weak nonlinearity, weak dispersion and weak perturbation in fluid mechanics in three spatial dimensions can be described by a generalized ( 3 + 1 )-dimensional variable-coefficient Kadomtsev–Petviashvili equation, which is studied in this paper with symbolic computation. Via the truncated Painlevé expansion, an auto-Bäcklund transformation is derived, based on which, under certain variable-coefficient constraints, one-soliton, two-soliton, homoclinic breather-wave and rouge-wave solutions are respectively obtained via the Hirota method. Graphic analysis shows that the soliton propagates with the varying soliton direction. Change of the value of any one of g ( t ), m ( t ), n ( t ), h ( t ), q ( t ) and l ( t ) in the equation can cause the change of the soliton shape, while the soliton amplitude cannot be affected by that change, where g ( t ) represents the dispersion, m ( t ) and n ( t ) respectively stand for the disturbed wave velocities along the y and z directions, h ( t ), q ( t ) and l ( t ) are the perturbed effects, y and z are the scaled spatial coordinates, and t is the temporal coordinate. Soliton direction and type of the interaction between the two solitons can vary with the change of the value of g ( t ), while they cannot be affected by m ( t ), n ( t ), h ( t ), q ( t ) and l ( t ) . Homoclinic breather wave and rouge wave are respectively displayed, where the rouge wave comes from the extreme behaviour of the homoclinic breather wave.