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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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dc.contributor.author Rabei, Eqab M.
dc.contributor.author Al-Jamel, A.
dc.contributor.author Widyan, H.
dc.contributor.author Baleanu, Dumitru
dc.date.accessioned 2020-05-11T13:30:59Z
dc.date.available 2020-05-11T13:30:59Z
dc.date.issued 2014-03
dc.identifier.issn 0022-2488
dc.identifier.issn 1089-7658
dc.identifier.uri http://hdl.handle.net/20.500.12416/3693
dc.description.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. tr_TR
dc.language.iso eng tr_TR
dc.publisher Amer Inst Physics tr_TR
dc.relation.isversionof 10.1063/1.4868479 tr_TR
dc.rights info:eu-repo/semantics/openAccess tr_TR
dc.subject Formulation tr_TR
dc.title Comment On "Maxwell's Equations And Electromagnetic Lagrangian Density in Fractional Form" [J. Math. Phys. 53, 033505 ( 2012)] tr_TR
dc.type editorial tr_TR
dc.relation.journal Journal of Mathematical Physics tr_TR
dc.contributor.authorID 56389 tr_TR
dc.identifier.volume 55 tr_TR
dc.identifier.issue 3 tr_TR
dc.contributor.department Çankaya Üniversitesi, Fen Edebiyat Fakültesi, Matematik Bölümü tr_TR


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