期刊
NONLINEAR DYNAMICS
卷 110, 期 1, 页码 693-704出版社
SPRINGER
DOI: 10.1007/s11071-022-07647-5
关键词
Generalized two-mode evolution equation; Simplified Hirota technique; Multiple solitons; Lump solution; Dependent variable transformation
资金
- SERB-DST, India [MTR/2020/000531]
- Research and Development Cell (RDC), Hansraj College, University of Delhi [HRC/RDC/2021/RP/16]
This article investigates a generalized two-mode evolution equation and examines its soliton solutions and interactions using logarithmic transformation and the Hirota method. The equations have applications in various real-life examples.
This article investigates a nonlinear fifth-order partial differential equation (PDE) in two-mode waves. The equation generalizes two-mode Sawada-Kotera (tmSK), two-mode Lax (tmLax), and two-mode Caudrey-Dodd-Gibbon (tmCDG) equations. In 2017, Wazwaz [1] presented three two-mode fifth-order evolutions equations as tmSK, tmLax, and tmCDG equations for the integrable two-mode KdV equation and established solitons up to three-soliton solutions. In light of the research above, we examine a generalized two-mode evolution equation using a logarithmic transformation concerning the equation's dispersion. It utilizes the simplified technique of the Hirota method to obtain the multiple solitons as a single soliton, two solitons, and three solitons with their interactions. Also, we construct one-lump solutions and their interaction with a soliton and depict the dynamical structures of the obtained solutions for solitons, lump, and their interactions. We show the 3D graphics with their contour plots for the obtained solutions by taking suitable values of the parameters presented in the solutions. These equations simultaneously study the propagation of two-mode waves in the identical direction with different phase velocities, dispersion parameters, and nonlinearity. These equations have applications in several real-life examples, such as gravity-affected waves or gravity-capillary waves, waves in shallow water, propagating waves in fast-mode and the slow-mode with their phase velocity in a strong and weak magnetic field, known as magneto-sound propagation in plasmas.
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