10.1007/s40096-021-00420-6

High-order exponentially fitted and trigonometrically fitted explicit two-derivative Runge–Kutta-type methods for solving third-order oscillatory problems

  1. Institute for Mathematical Research, Universiti Putra Malaysia, UPM Serdang, Selangor, 43400, MY
  2. Institute for Mathematical Research and Department of Mathematics and Statistics, Universiti Putra Malaysia, UPM Serdang, Selangor, 43400, MY
  3. Institute of Industry Revolution 4.0, The National University of Malaysia, UKM Bangi, Selangor, 43600, MY

Published in Issue 2021-07-23

How to Cite

Lee, K. C., Senu, N., Ahmadian, A., & Ibrahim, S. N. I. (2021). High-order exponentially fitted and trigonometrically fitted explicit two-derivative Runge–Kutta-type methods for solving third-order oscillatory problems. Mathematical Sciences, 16(3 (September 2022). https://doi.org/10.1007/s40096-021-00420-6

Abstract

Abstract Three stage sixth-order exponentially fitted and trigonometrically fitted explicit two-derivative Runge–Kutta-type methods are proposed for solving u′′′(t)=f(t,u(t),u′(t)).\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$u^{'''}(t) = \, f(t,u(t),u'(t)).$$\end{document} The idea of construction is based on linear composition of the set functions eωt\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$e^{\omega t}$$\end{document} and e-ωt\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$e^{-\omega t}$$\end{document} for exponentially fitted and eiωt\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$e^{i\omega t}$$\end{document} and e-iωt\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$e^{-i\omega t}$$\end{document} for trigonometrically fitted with ω∈R\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\omega \in \mathbb {R}$$\end{document} to integrate initial value problems. The selected coefficients of two-derivative Runge–Kutta-type method are modified to depend on the principle frequency of the numerical problems to construct exponentially fitted and trigonometrically fitted Runge–Kutta-type direct methods, denoted as EFTDRKT6 and TFTDRKT6 methods. The numerical experiments illustrate competence of the new exponentially fitted and trigonometrically fitted method compared to existing methods for solving special type third-order ordinary differential equations with initial value problems.

Keywords

  • Runge–Kutta-type methods,
  • Third-order oscillatory differential equations,
  • Initial value problems,
  • Exponentially fitted,
  • Trigonometrically fitted

References

  1. Gregus (1986) (pp. 257-258) D. Reidel Publishing Company
  2. Duffy and Wilson (1997) A third-order differential equation arising in thin-film flows and relevant to Tanner's Law (pp. 63-68) https://doi.org/10.1016/S0893-9659(97)00036-0
  3. Ignaczak (2009) Modeling heat transfer in metal films by a third-order derivative-in-time dissipative and dispersive wave equation (pp. 847-861) https://doi.org/10.1080/01495730802637548
  4. Mirzabeigy and Yildirim (2014) Approximate periodic solution for nonlinear jerk equation as a third-order nonlinear equation via modified differential transform method (pp. 622-633) https://doi.org/10.1108/EC-02-2012-0024
  5. Yang, Y., Fang, Y., You, X., Wang, B.: Novel exponentially fitted two-derivative runge-kutta methods with equation-dependent coefficients for first-order differential equations. Dis. Dyn. Nat. Soc., Article ID 9827952 (2016)
  6. Abdulganiy (2018) Trigonometrically fitted block backward differentiation methods for first order initial value problems with periodic solution (pp. 1-4) https://doi.org/10.9734/JAMCS/2018/42774
  7. Monovasilis et al. (2015) Construction of exponentially fitted symplectic Runge-Kutta-nystrom methods from partitioned Runge-Kutta methods (pp. 1923-1930)
  8. Ngwane, F.F., Jator, S.N.: A Trigonometrically fitted block method for solving oscillatory second-order initial value problems and hamiltonian systems. J. Appl. Math., Article ID 4029371 (2018)
  9. Chen, B.Z., Zhai, W.J.: Implicit symmetric and symplectic exponentially fitted modified Runge-Kutta-Nystrom methods for solving oscillatory problems. J. Inequalit. Appl. (2018).
  10. https://doi.org/10.1186/s13660-018-1915-4
  11. Ghawadri, N., Senu, S., Ismail, F., Ibrahim, Z.B.: Exponentially fitted and trigonometrically fitted explicit modified Runge-Kutta type methods for solving
  12. y″′(x)=f(x,y,y′)
  13. usepackage{amsmath}
  14. usepackage{wasysym}
  15. usepackage{amsfonts}
  16. usepackage{amssymb}
  17. usepackage{amsbsy}
  18. usepackage{mathrsfs}
  19. usepackage{upgreek}
  20. setlength{oddsidemargin}{-69pt}
  21. begin{document}$$y^{prime prime prime }(x) = , f(x,y,y^{prime })$$end{document}]]>
  22. . J. Appl. Math., Article ID 4029371 (2018)
  23. Samat, F., Ismail, E.S.: Variable step exponentially fitted explicit sixth-order hybrid method with four stages for spring-mass and other oscillatory problems. Symmetry
  24. 12
  25. , (2020).
  26. https://doi.org/10.3390/sym12030387
  27. Lazer (1966) The Behavior of Solutions of the Differential Equation y″′+p(x)y′+q(x)y=0documentclass[12pt]{minimal}
  28. usepackage{amsmath}
  29. usepackage{wasysym}
  30. usepackage{amsfonts}
  31. usepackage{amssymb}
  32. usepackage{amsbsy}
  33. usepackage{mathrsfs}
  34. usepackage{upgreek}
  35. setlength{oddsidemargin}{-69pt}
  36. begin{document}$$y^{prime prime prime }+p(x)y^{prime }+q(x)y = , 0$$end{document} (pp. 435-466) https://doi.org/10.2140/pjm.1966.17.435
  37. Lee, K.C., Senu, N., Ahmadian, A., Ibrahim, S.N.I.: Numerical study of third-order ordinary differential equations using a new class of two derivative Runge-Kutta type methods. Alexandria Eng. J. (2020).
  38. https://doi.org/10.1016/j.aej.2020.03.008
  39. Al-Shimmary (2017) Solving Initial Value Problem Using Runge-Kutta 6-th Order Method (pp. 3953-3961)
  40. Hussain, K.A.: Trigonometrically fitted fifth-order explicit two-derivative Runge-Kutta method with FSAL property. J. Phys. Conf. Ser.
  41. 1294
  42. , (2019).
  43. https://doi.org/10.1088/1742-6596/1294/3/032009
  44. Ahmad et al. (2019) Trigonometrically-fitted higher order two derivative Runge-Kutta method for solving orbital and related periodical IVPs (pp. 1312-1323)
  45. Kumar and Singh (2012) Phase plane analysis and traveling wave solution of third order nonlinear singular problems arising in thin film evolution (pp. 2886-2895) https://doi.org/10.1016/j.camwa.2012.05.003
  46. Kulken (1996) A third-order differential equation arising in thin-film flows and relevant to Tanner's law (pp. 63-68)
  47. Morlando, F.: Approximate analytical solution of a third-order ivp arising in thin film flows driven by surface tension. Boletim da Sociedade Paranaense de Matematica
  48. 35
  49. , (2015).
  50. https://doi.org/10.5269/bspm.v35i3.28349
  51. Allogmany, R., Ismail, F.: Implicit three-point block numerical algorithm for solving third order initial value problem directly with applications. Mathematics
  52. 8
  53. , (2020).
  54. https://doi.org/10.3390/math8101771