Variational iteration method for solving coupled nonlinear system of Klein-Gordon equations
Abstract
In this paper, variational iteration technique is applied to solve nonlinear coupled Klein-Gordon equations (CNLKGE). The equations arise when dealing with particle physics. The numerical solutions of CNLKGE have been compared to the exact solutions and presented graphically. The results of the proposed method are in good agreement with the exact solutions provided by [1]. The suggested algorithm is efficient and easier to employ compared to other methods like the perturbation method.
Full Text
Tables and figures are in the full-text PDF.
Introduction
Over the last few decades, searching for exact and numerical solutions of nonlinear partial differential equations has become an interesting area in the physical, biological sciences and nonlinear sciences [9,10] . In order to deeper understanding of these nonlinear phenomena, several mathematicians, engineers and scientists make the effort to seek more accurate solutions. The nonlinear coupled Klein-Gordon equation (CNLKGE) arises in the area of particle physics. Spin zero particles can be explained using CNLKGE. That is like π -meson and so on. The Nonlinear coupled Klein-Gordon equation was first studied by [1][2][3] respectively. Recently, [7] solved closely related equation called Schrodinger-Klein-Gordon equation using Variational Iteration Method (VIM). In this paper, our aim is to develop VIM for CNLKGE and compare the solutions with the exact solutions given by [1] . In 1999, the Variational Iteration Method (VIM) was first time proposed by J.H. He 1999He , 2007He , 1998 [4-6] [4-6] . The method does not require any transformation, discretization, perturbation or any restrictive assumptions that are used to handle nonlinear terms as may be needed by other methods. The structure of this article are sequenced as; Section II gives basics of VIM. Section III develops the recursive algorithms for CNLKGE. Section IV tabulates and analyze the absolute errors. Section V concludes the study. The system to be solved is defined by;
with the derived initial conditions
Variational Iteration Method (VIM) 2.1 Concepts of VIM
Consider the following generalized system. According to [4,8] , to use variational iteration method (VIM), the system is expressed in the following format.
The correction functional for equations ( 6) and ( 7) can be written as
Where 1 () and 2 () are Lagrangian multipliers to be determined using variational theory, , nn uv are considered as restricted variations i.e.
0, 0
Equations ( 8) and ( 9) are called correction functional for equations ( 6) and ( 7) respectively. The solutions can now be found using limit definitions;
Numerical Solution of CNLKGE using VIM
Particularly, the correction functionals for our equations ( 1) and ( 2) are given by
By making the correction functionals stationary, we get 1 () t and 2 ( ) 1
We obtain the iterative formulae
Are the initial conditions of our system given by equations ( 1) and (2) Using the variational iteration formulae equations ( 12) and ( 13) along the t direction we generated the approximants.
We iterated two times to get; 1 1 2 ,, u v u and 2 v . From equations ( 16), ( 17), ( 18), ( 19), ( 20) and ( 21) solutions are can now be found by the limits;
( , ) lim ( , ) These solutions obtained from equations ( 22) and ( 23) are used for numerical study of convergence of VIM [11] .
Numerical Results and Discussions
In this proposed method, 0.5, c for analysis purposes. The actual expressions for equations ( 22) and ( 23) are extremely long and cannot be shown here. From Fig. 1, the convergence of VIM is rapid. The errors are in the order of 1E-4. It is computationally efficient. At the second iteration, the absolute errors dropped drastically to almost zero. From Fig. 2, the convergence is good. When Fig. 1 and Fig. 2 are compared, it was noted that ( , ) u x t values converged more rapidly than the ( , ) v x t values. Absolute errors become smaller as you increase the number of iterations.
First iteration of VIM
Summary of Findings
In this study, VIM has been used to compute the semi-analytic solution of the simultaneous nonlinear Klein-Gordon equations.
Results obtained by VIM were in an good agreement with the exact results obtained by [1] . This therefore showed that the method is efficient and reliable. VIM do not use small parameter like in homotopy method. VIM reduces the errors as we progress in the iterations. VIM can be used to solve nonlinear problems efficiently compared to Finite Difference method. Based on its accuracy, VIM can be utilized to solve linear and non-linear problems. This explains why a few approximations can be used to achieve a high degree of accuracy. From the tables 1-4 and Fig. 1 and Fig. 2 we concluded that accuracy is improved as more iterations are used. The computations in this paper were performed using MATLAB 6.1 symbolic toolbox.
Conflict of interests
The author (s) declare that there is no conflict of interests.
References
Cited by 5
From OpenAlex, OpenCitations and reference lists read by Scinovex
- Adomian Decomposition and Variational Iteration Methods in the Context of Partial Differential Equations ↗
Khadeejah James Audu, Lawrence Linus, Yusuph Amuda Yahaya, Sikirulai Abolaji Akande · Journal of Innovative Science and Engineering (JISE) · 2025
Partial Differential Equations (PDE) help model problems in science and engineering, given their abilities to capture complex phenomena compared to Ordinary Differential Equations. This paper aims to investigate two semi-analytical techniques called the Adomian Decomposition Method (ADM) and the Variational Iteration Method (VIM), how these methods can be used in practice, and to make a comparative study of the two…
❝ 0PDF - Semi-classical lattice Boltzmann model for dissipative quantum plasma flow ↗
W. Choe, Suk Kim, Y.-J. Kim, Yong-Jun Kim, J. S. Kim · International Journal of Advanced Academic Studies · 2025
A semi-classical lattice Boltzmann model for quantum plasma flow is proposed based on the Wigner-Fokker-Planck equation coupled with Poisson’s equation. We derive the discrete quantum kinetic equation with operator terms series-expanded by Hermitian polynomials and present the semi-classical lattice Boltzmann equation that guarantees numerical stability. Numerical experiments are performed on electron fluid in dense quantum plasma, which are typically generated
- Relativistic laser pulse dynamics in dense quantum plasma by QED approach ↗
Punit Kumar · International Journal of Physics and Applications · 2024
Utilizing the covariant Lagrangian function and Euler-Lagrange equation, a set of Dirac equations has been derived to elucidate the interaction between strong electromagnetic waves and spin-polarized plasmas. Analysis reveals that relativistic effects significantly impact the interaction process, manifesting through three key factors: self-energy, vacuum polarization, and radiation reaction. In this specific research paper, a quantum electrodynamical approach has been employed
- Investigation of three body system using confining potential in non-relativistic quark model ↗
Rakesh Kumar Paswan, Sanjeet Kumar · International Journal of Physics and Mathematics · 2024
This paper investigates the properties of three-body baryonic systems using a non-relativistic quark model with a confining potential. The objective is to understand the binding energies and mass spectra of light and heavy baryons, such as protons, neutrons, and their excited states. The research employs a potential that combines a short-range Coulomb-like term, derived from one-gluon exchange, and a long-range
- Genetic algorithms molecular effect model optimization computational method for high temperature superconductors ↗
Francisco Casesnoves · International Journal of Engineering in Computer Science · 2023
Genetic algorithms software was applied in 3D Graphical and Interior Optimization methods for two High Temperature Superconductors (HTSCs) classes. Namely, Tin (Sn) class with [TC > 0°] and Thallium (Tl) one subject to [TC ˂ 0°, TC > 0°] in Molecular Effect Model (MEM). Results comprise Tikhonov Regularization Functional mathematical algorithms for these HTSCs group without using logarithmic changes. Results
How this paper connects to the literature. Drag to explore, click any node to open that paper.
