Comment on "maxwell's Equations and Electromagnetic Lagrangian Density in Fractional Form" [J. Math. Phys. 53, 033505 ( 2012)]
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Date
2014
Journal Title
Journal ISSN
Volume Title
Publisher
Amer inst Physics
Open Access Color
BRONZE
Green Open Access
No
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Publicly Funded
No
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

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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