2004
DOI: 10.1088/0264-9381/21/21/007
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Counterrotating perfect fluid discs as sources of electrovacuum static spacetimes

Abstract: The interpretation of some electrovacuum spacetimes in terms of counterrotating perfect fluid discs is presented. The interpretation is made by means of an ‘inverse problem’ approach used to obtain disc sources of known static solutions of the Einstein–Maxwell equations. In order to do such an interpretation, a detailed study is presented of the counterrotating model (CRM) for generic electrovacuum static axially symmetric relativistic thin discs with nonzero radial pressure. Four simple families of models of … Show more

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Cited by 15 publications
(26 citation statements)
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“…On the other hand, thin disks have been discussed as sources for Kerr-Newman fields [32,33], magnetostatic axisymmetric fields [34,35], and conformastatic and conformastationary metrics [36][37][38]. Also, models of electrovacuum static counterrotating dust disks were presented in [39], charged perfect fluid disks were studied in [40], and charged perfect fluid disks as sources of static and Taub-NUT-type spacetimes in [41,42]. Also, monopole and dipole layers in curved spacetimes were analyzed in [43], and electromagnetic sources distributed on shells in a Schwarzschild background in [44].…”
Section: Introductionmentioning
confidence: 99%
“…On the other hand, thin disks have been discussed as sources for Kerr-Newman fields [32,33], magnetostatic axisymmetric fields [34,35], and conformastatic and conformastationary metrics [36][37][38]. Also, models of electrovacuum static counterrotating dust disks were presented in [39], charged perfect fluid disks were studied in [40], and charged perfect fluid disks as sources of static and Taub-NUT-type spacetimes in [41,42]. Also, monopole and dipole layers in curved spacetimes were analyzed in [43], and electromagnetic sources distributed on shells in a Schwarzschild background in [44].…”
Section: Introductionmentioning
confidence: 99%
“…These solutions, in the vacuum and static case, correspond to the Morgan and Morgan solutions [2]. A more general class of solutions representating finite thin disks can be constructed using a method based on the use of conformal transformations and solving a boundaryvalue problem [3,6,4,12,23,24].…”
Section: Electrovacuum Rotating Relativistic Thin Disksmentioning
confidence: 99%
“…Now, can happen that the obtained solutions do not satisfy any of these two conditions. That is, the counterrotating velocities are, in general, not completely determined by the constraint (30). Thus, the CRM is in general undetermined since the counterrotaing energy densities and pressures can not be explicitly written without a knowledge of the counterrotating tangential velocities.…”
Section: Counterrotating Charged Dust Disksmentioning
confidence: 99%