New form of the Kerr-Newman solution
Michael Hobson

TL;DR
This paper introduces a new coordinate system for the Kerr-Newman black hole solution that is well-behaved at horizons and adaptable to different charge configurations, providing a unified and extended description of the spacetime.
Contribution
The authors develop a novel coordinate system for the Kerr-Newman solution that generalizes Doran and Eddington-Finkelstein coordinates, offering a global and physically intuitive description of charged rotating black holes.
Findings
Coordinates reduce to Doran coordinates when charge is zero.
Range of validity extends with increasing charge magnitude.
Coordinates become Eddington-Finkelstein in the limit of large charge.
Abstract
A new form of the Kerr-Newman solution is presented. The solution involves a time coordinate which represents the local proper time for a charged massive particle released from rest at spatial infinity. The chosen coordinates ensure that the solution is well-behaved at horizons and enable an intuitive description of many physical phenomena. If the charge of the particle , the coordinates reduce to Doran coordinates for the Kerr solution with the replacement , where and are the mass and charge of the black hole, respectively. Such coordinates are valid only for , however, which corresponds to the region that a neutral particle released from rest at infinity can penetrate. By contrast, for and of opposite sign to , the new coordinates have a progressively extended range of validity as increases and tend to advanced…
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Taxonomy
TopicsAstrophysical Phenomena and Observations · Black Holes and Theoretical Physics · Relativity and Gravitational Theory
