4.3 Article

A study of travelling, periodic, quasiperiodic and chaotic structures of perturbed Fokas-Lenells model

Journal

PRAMANA-JOURNAL OF PHYSICS
Volume 95, Issue 1, Pages -

Publisher

INDIAN ACAD SCIENCES
DOI: 10.1007/s12043-020-02067-9

Keywords

Perturbed Fokas-Lenells model; GM; expansion method; bifurcation analysis; 02; 20; Sv; 02; 30; Jr; 11; 30; i; 47; 20; Ky

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In this paper, a diverse range of travelling wave structures of perturbed Fokas-Lenells model (p-FLM) is obtained using the extended (G ' /G2)-expansion technique, with the existence of solutions guaranteed by reporting constraint conditions. The governing model is then converted into a planer dynamical system through Gallelian transformation, with phase portraits plotted for pertinent parameters. The study also uses the Runge-Kutta fourth-order technique to extract nonlinear periodic solutions and analyzes quasiperiodic and chaotic behavior for different parameter values after introducing an external periodic force.
In this paper, a diverse range of travelling wave structures of perturbed Fokas-Lenells model (p-FLM) is obtained by using the extended (G ' /G2)-expansion technique. The existence of the obtained solutions is guaranteed by reporting constraint conditions. Then, the governing model is converted into the planer dynamical system with the help of Gallelian transformation. Every possible form of phase portraits is plotted for pertinent parameters, viz. k,beta ,d1,d2,d3. We also used the Runge-Kutta fourth-order technique to extract the nonlinear periodic solutions of the considered problem and outcomes are presented graphically. Furthermore, quasiperiodic and chaotic behaviour of p-FLM is analysed for different values of parameters after deploying an external periodic force. Quasiperiodic-chaotic nature is observed for selected values of parameters k,beta ,d1,d2,d3 by keeping the force and frequency of the perturbed dynamical system fixed. The sensitive analysis is employed on some initial value problems (IVPs). It is seen that de-sensitisation is present in the perturbed dynamical system while for the same values of parameters, the unperturbed dynamical system has a nonlinear periodic solution.

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