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Comment on "maxwell's Equations and Electromagnetic Lagrangian Density in Fractional Form" [J. Math. Phys. 53, 033505 ( 2012)]

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Date

2014

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Volume Title

Publisher

Amer inst Physics

Open Access Color

BRONZE

Green Open Access

No

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Abstract

In a recent paper, Jaradat et al. [J. Math. Phys. 53, 033505 (2012)] have presented the fractional form of the electromagnetic Lagrangian density within the Riemann-Liouville fractional derivative. They claimed that the Agrawal procedure [O. P. Agrawal, J. Math. Anal. Appl. 272, 368 (2002)] is used to obtain Maxwell's equations in the fractional form, and the Hamilton's equations of motion together with the conserved quantities obtained from fractional Noether's theorem are reported. In this comment, we draw the attention that there are some serious steps of the procedure used in their work are not applicable even though their final results are correct. Their work should have been done based on a formulation as reported by Baleanu and Muslih [Phys. Scr. 72, 119 (2005)]. (C) 2014 AIP Publishing LLC.

Description

Al-Jamel, Ahmed/0000-0003-1801-610X; Widyan, Hatem/0000-0001-7663-4649

Keywords

Lagrangian formalism and Hamiltonian formalism in mechanics of particles and systems, Hamilton's equations, Fractional derivatives and integrals, Electromagnetic theory (general), fractional Noether's theorem, Maxwell's equations in the fractional form, Riemann-Liouville fractional derivative, Symmetries and conservation laws in mechanics of particles and systems, Agrawal procedure

Fields of Science

0103 physical sciences, 0101 mathematics, 01 natural sciences

Citation

WoS Q

Q3

Scopus Q

Q3
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OpenCitations Citation Count
2

Source

Journal of Mathematical Physics

Volume

55

Issue

3

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CrossRef : 2

Scopus : 2

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Mendeley Readers : 4

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