Implicit symmetric and symplectic exponentially fitted modified Runge–Kutta–Nyström methods for solving oscillatory problems
Abstract Symplectic exponentially fitted RK and RKN methods have been extensively studied by many researchers. Due to their good property, they have been applied to many problems such as pendulum, Morse oscillator, harmonic oscillator, Lennard–Jones oscillator, Kepler’s orbit problem, and so on. In...
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doaj-72edf5fd8c8d40ffbc60061840c500602020-11-25T01:34:07ZengSpringerOpenJournal of Inequalities and Applications1029-242X2018-11-012018111710.1186/s13660-018-1915-4Implicit symmetric and symplectic exponentially fitted modified Runge–Kutta–Nyström methods for solving oscillatory problemsBing Zhen Chen0Wen Juan Zhai1School of Science, Beijing Jiaotong UniversityDepartment of Mathematics, Beijing Jiaotong University Haibin CollegeAbstract Symplectic exponentially fitted RK and RKN methods have been extensively studied by many researchers. Due to their good property, they have been applied to many problems such as pendulum, Morse oscillator, harmonic oscillator, Lennard–Jones oscillator, Kepler’s orbit problem, and so on. In this paper, we construct an implicit symmetric and symplectic exponentially fitted modified Runge–Kutta–Nyström (ISSEFMRKN) method. The new integrator integrates exactly differential systems whose solutions can be expressed as linear combinations of functions from the set {exp(λt),exp(−λt)} $\{\exp(\lambda t),\exp(-\lambda t)\}$, λ∈C $\lambda\in\mathbb{C}$, or equivalently {sin(ωt),cos(ωt)} $\{\sin(\omega t),\cos(\omega t)\}$ when λ=iω $\lambda=i\omega$, ω∈R $\omega \in\mathbb{R}$. When z=λh $z=\lambda h$ approaches zero, the ISSEFMRKN method reduces to the classical symplectic, symmetric RKN integrator. Numerical experiments are accompanied to show the efficiency and competence of the new method compared with some efficient codes in the literature.http://link.springer.com/article/10.1186/s13660-018-1915-4ImplicitSymmetricSymplecticExponentially fittedModified Runge–Kutta–Nyström methodOscillatory problem |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Bing Zhen Chen Wen Juan Zhai |
spellingShingle |
Bing Zhen Chen Wen Juan Zhai Implicit symmetric and symplectic exponentially fitted modified Runge–Kutta–Nyström methods for solving oscillatory problems Journal of Inequalities and Applications Implicit Symmetric Symplectic Exponentially fitted Modified Runge–Kutta–Nyström method Oscillatory problem |
author_facet |
Bing Zhen Chen Wen Juan Zhai |
author_sort |
Bing Zhen Chen |
title |
Implicit symmetric and symplectic exponentially fitted modified Runge–Kutta–Nyström methods for solving oscillatory problems |
title_short |
Implicit symmetric and symplectic exponentially fitted modified Runge–Kutta–Nyström methods for solving oscillatory problems |
title_full |
Implicit symmetric and symplectic exponentially fitted modified Runge–Kutta–Nyström methods for solving oscillatory problems |
title_fullStr |
Implicit symmetric and symplectic exponentially fitted modified Runge–Kutta–Nyström methods for solving oscillatory problems |
title_full_unstemmed |
Implicit symmetric and symplectic exponentially fitted modified Runge–Kutta–Nyström methods for solving oscillatory problems |
title_sort |
implicit symmetric and symplectic exponentially fitted modified runge–kutta–nyström methods for solving oscillatory problems |
publisher |
SpringerOpen |
series |
Journal of Inequalities and Applications |
issn |
1029-242X |
publishDate |
2018-11-01 |
description |
Abstract Symplectic exponentially fitted RK and RKN methods have been extensively studied by many researchers. Due to their good property, they have been applied to many problems such as pendulum, Morse oscillator, harmonic oscillator, Lennard–Jones oscillator, Kepler’s orbit problem, and so on. In this paper, we construct an implicit symmetric and symplectic exponentially fitted modified Runge–Kutta–Nyström (ISSEFMRKN) method. The new integrator integrates exactly differential systems whose solutions can be expressed as linear combinations of functions from the set {exp(λt),exp(−λt)} $\{\exp(\lambda t),\exp(-\lambda t)\}$, λ∈C $\lambda\in\mathbb{C}$, or equivalently {sin(ωt),cos(ωt)} $\{\sin(\omega t),\cos(\omega t)\}$ when λ=iω $\lambda=i\omega$, ω∈R $\omega \in\mathbb{R}$. When z=λh $z=\lambda h$ approaches zero, the ISSEFMRKN method reduces to the classical symplectic, symmetric RKN integrator. Numerical experiments are accompanied to show the efficiency and competence of the new method compared with some efficient codes in the literature. |
topic |
Implicit Symmetric Symplectic Exponentially fitted Modified Runge–Kutta–Nyström method Oscillatory problem |
url |
http://link.springer.com/article/10.1186/s13660-018-1915-4 |
work_keys_str_mv |
AT bingzhenchen implicitsymmetricandsymplecticexponentiallyfittedmodifiedrungekuttanystrommethodsforsolvingoscillatoryproblems AT wenjuanzhai implicitsymmetricandsymplecticexponentiallyfittedmodifiedrungekuttanystrommethodsforsolvingoscillatoryproblems |
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1725073579780866048 |