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Charged Shear-Free Fluids and Complexity in First Integrals

The equation [Formula: see text] is the charged generalization of the Emden-Fowler equation that is crucial in the study of spherically symmetric shear-free spacetimes. This version arises from the Einstein–Maxwell system for a charged shear-free matter distribution. We integrate this equation and f...

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Detalles Bibliográficos
Autores principales: Gumede, Sfundo C., Govinder, Keshlan S., Maharaj, Sunil D.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9140625/
https://www.ncbi.nlm.nih.gov/pubmed/35626530
http://dx.doi.org/10.3390/e24050645
Descripción
Sumario:The equation [Formula: see text] is the charged generalization of the Emden-Fowler equation that is crucial in the study of spherically symmetric shear-free spacetimes. This version arises from the Einstein–Maxwell system for a charged shear-free matter distribution. We integrate this equation and find a new first integral. For this solution to exist, two integral equations arise as integrability conditions. The integrability conditions can be transformed to nonlinear differential equations, which give explicit forms for [Formula: see text] and [Formula: see text] in terms of elementary and special functions. The explicit forms [Formula: see text] and [Formula: see text] arise as repeated roots of a fourth order polynomial. This is a new solution to the Einstein-Maxwell equations. Our result complements earlier work in neutral and charged matter showing that the complexity of a charged self-gravitating fluid is connected to the existence of a first integral.