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N ‐lump and interaction solutions of localized waves to the (2 + 1)‐dimensional asymmetrical Nizhnik–Novikov–Veselov equation arise from a model for an incompressible fluid
Author(s) -
Manafian Jalil,
Ilhan Onur Alp,
Avazpour Ladan,
Alizadeh As'ad
Publication year - 2020
Publication title -
mathematical methods in the applied sciences
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.719
H-Index - 65
eISSN - 1099-1476
pISSN - 0170-4214
DOI - 10.1002/mma.6665
Subject(s) - breather , soliton , mathematics , limit (mathematics) , bilinear interpolation , bilinear form , nonlinear system , compressibility , mathematical analysis , operator (biology) , rogue wave , classical mechanics , mathematical physics , physics , quantum mechanics , mechanics , biochemistry , statistics , chemistry , repressor , transcription factor , gene
The present article deals with M ‐soliton solution and N ‐soliton solution of the (2 + 1)‐dimensional asymmetrical Nizhnik–Novikov–Veselov equation by virtue of Hirota bilinear operator method. The obtained solutions for solving the current equation represent some localized waves including soliton, breather, lump, and their interactions, which have been investigated by the approach of the long‐wave limit. Mainly, by choosing the specific parameter constraints in the M ‐soliton and N ‐soliton solutions, all cases of the one breather or one lump can be captured from the two, three, four, and five solitons. In addition, the performances of the mentioned technique, namely, the Hirota bilinear technique, are substantially powerful and absolutely reliable to search for new explicit solutions of nonlinear models. Meanwhile, the obtained solutions are extended with numerical simulation to analyze graphically, which results in localized waves and their interaction from the two‐, three‐, four‐, and five‐soliton solutions profiles. They will be extensively used to report many attractive physical phenomena in the fields of acoustics, heat transfer, fluid dynamics, classical mechanics, and so on.