Abstract

In this new work, the free motion of a coupled oscillator is investigated. First, a fully description of the system under study is formulated by considering its classical Lagrangian, and as a result, the classical Euler-Lagrange equations of motion are constructed. After this point, we extend the classical Lagrangian in fractional sense, and thus, the fractional Euler-Lagrange equations of motion are derived. In this new formulation, we consider a recently introduced fractional operator with Mittag-Leffler nonsingular kernel. We also present an efficient numerical method for solving the latter equations in a proper manner. Due to this new powerful technique, we are able to obtain remarkable physical thinks; indeed, we indicate that the complex behavior of many physical systems is realistically demonstrated via the fractional calculus modelling. Finally, we report our numerical findings to verify the theoretical analysis.

Highlights

  • There are two main approaches in the classical mechanics to get the equations of motion for a dynamical system: Newtonian and Lagrangian

  • We investigate the dynamical behavior of the fractional Euler-Lagrange equations (FELEs) of motion for the coupled oscillator expressed by Equations (17)–(18) considering different values of the fractional order q

  • This paper studied the concept of the fractional calculus (FC) to evaluate the equations of motion for a coupled oscillator

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Summary

Introduction

There are two main approaches in the classical mechanics to get the equations of motion for a dynamical system: Newtonian and Lagrangian. The second approach was invented by Joseph Louis Lagrange, a French Mathematician. This approach is considered as a useful technique to find the equations of motion for many kinds of physical processes [1]. The fractional calculus (FC) is a branch of mathematical analysis, which deals with the non-integer integral and derivative operators. Over the past few decades, the classical mechanics has been extended by using the new aspects of the FC. In Riewe [10], the non-conservative Lagrangian systems were studied by Riewe using the concept of the FC. In Laskin [12], he developed the fractional quantum mechanics

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