An Efficient Technique of Fractional-Order Physical Models Involving ρ-Laplace Transform

Nehad Ali Shah, Ioannis Dassios, Essam R. El-Zahar, Jae Dong Chung

Research output: Contribution to journalArticlepeer-review

8 Scopus citations

Abstract

In this article, the ρ-Laplace transform is paired with a new iterative method to create a new hybrid methodology known as the new iterative transform method (NITM). This method is applied to analyse fractional-order third-order dispersive partial differential equations. The suggested technique procedure is straightforward and appealing, and it may be used to solve non-linear fractional-order partial differential equations effectively. The Caputo operator is used to express the fractional derivatives. Four numerical problems involving fractional-order third-order dispersive partial differential equations are presented with their analytical solutions. The graphs determined that their findings are in excellent agreement with the precise answers to the targeted issues. The solution to the problems at various fractional orders is achieved and found to be correct while comparing the exact solutions at integer-order problems. Although both problems are the non-linear fractional system of partial differential equations, the present technique provides its solution sophisticatedly. Including both integer and fractional order issues, solution graphs are carefully drawn. The fact that the issues’ physical dynamics completely support the solutions at both fractional and integer orders is significant. Moreover, despite using very few terms of the series solution attained by the present technique, higher accuracy is observed. In light of the various and authentic features, it can be customized to solve different fractional-order non-linear systems in nature.
Original languageAmerican English
JournalMathematics
Volume10
Issue number5
DOIs
StatePublished - 1 Mar 2022

Keywords

  • Approximate solution
  • Caputo’s derivative
  • New iterative method
  • Third-order dispersive equations
  • ρ-Laplace transform

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