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Magnetohydrodynamics in stationary and axisymmetric spacetimes: a fully covariant approach

General Relativity and Quantum Cosmology · Submitted 18 Jan 2011

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim In particular, we present the first relativistic version of the Soloviev transfield equation, subcases of which lead to fully covariant versions of the Grad-Shafranov equation and of the Stokes equation in the hydrodynamical limit.

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arXiv ID1101.3497 (version 2)
Pith IDPPWDKZC4, Pith's permanent record of this paper and its review
CitationCharalampos Markakis, Eric Gourgoulhon, Koji Uryu, Yoshiharu Eriguchi. "Magnetohydrodynamics in stationary and axisymmetric spacetimes: a fully covariant approach." arXiv:1101.3497 (2011). https://pith.science/paper/PPWDKZC4
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What the abstract itself states, as probabilities: claims first 0.89 · states limitation 0.24 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.03 · compares with prior results 0.84 · mentions code or data availability 0.02.

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arXiv listing abstract v2. Results and the main claim are underlined; .

A fully geometrical treatment of general relativistic magnetohydrodynamics (GRMHD) is developed under the hypotheses of perfect conductivity, stationarity and axisymmetry. The spacetime is not assumed to be circular, which allows for greater generality than the Kerr-type spacetimes usually considered in GRMHD. Expressing the electromagnetic field tensor solely in terms of three scalar fields related to the spacetime symmetries, we generalize previously obtained results in various directions. In particular, we present the first relativistic version of the Soloviev transfield equation, subcases of which lead to fully covariant versions of the Grad-Shafranov equation and of the Stokes equation in the hydrodynamical limit. We have also derived, as another subcase of the relativistic Soloviev equation, the equation governing magnetohydrodynamical equilibria with purely toroidal magnetic fields in stationary and axisymmetric spacetimes.

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What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 A fully geometrical treatment of general relativistic magnetohydrodynamics (GRMHD) is developed under the hypotheses of perfect conductivity, stationarity and axisymmetry. contribution 0.96 0.93 0.15 asserted 1.00
s1 The spacetime is not assumed to be circular, which allows for greater generality than the Kerr-type spacetimes usually considered in GRMHD. contribution 0.66 0.50 0.06 asserted 0.98
s2 Expressing the electromagnetic field tensor solely in terms of three scalar fields related to the spacetime symmetries, we generalize previously obtained results in various directions. method 0.51 0.93 0.16 asserted 1.00
s3 In particular, we present the first relativistic version of the Soloviev transfield equation, subcases of which lead to fully covariant versions of the Grad-Shafranov equation and of the Stokes equation in the hydrodynamical limit. result 0.62 0.95 0.47 asserted 1.00
s4 We have also derived, as another subcase of the relativistic Soloviev equation, the equation governing magnetohydrodynamical equilibria with purely toroidal magnetic fields in stationary and axisymmetric spacetimes. result 0.80 0.97 0.13 asserted 1.00

What kind of paper the classifier reports this is: theoretical result 0.99 · evidence from proof or derivation 1.00.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

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Original abstract

A fully geometrical treatment of general relativistic magnetohydrodynamics (GRMHD) is developed under the hypotheses of perfect conductivity, stationarity and axisymmetry. The spacetime is not assumed to be circular, which allows for greater generality than the Kerr-type spacetimes usually considered in GRMHD. Expressing the electromagnetic field tensor solely in terms of three scalar fields related to the spacetime symmetries, we generalize previously obtained results in various directions. In particular, we present the first relativistic version of the Soloviev transfield equation, subcases of which lead to fully covariant versions of the Grad-Shafranov equation and of the Stokes equation in the hydrodynamical limit. We have also derived, as another subcase of the relativistic Soloviev equation, the equation governing magnetohydrodynamical equilibria with purely toroidal magnetic fields in stationary and axisymmetric spacetimes.

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3 arXiv papers cite this in 3 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 2 sentences without a confident label

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What it cites · 2 sentences without a confident label

Cites as background 2 papers
  • General relativistic magnetohydrodynamics (GRMHD) is a rapidly developing field of modern astrophysics [ref] , driven by numerous observations of accretion disks around black holes [ref] , jets in active galactic nuclei or microquasars [ref] , gamma ray bursts, hypernovae, pulsars [ref] and strongly magnetized neutrons stars (magnetars).

    Magnetic acceleration of relativistic jets · Introduction · 0.99

  • We assume that the spacetime $(,g)$ possesses two symmetries: (i) stationarity: there exists a group action of $(,+)$ on $$ whose orbits are timelike curves and which leaves $g$ invariant; (ii) axisymmetry: there exists a group action of $SO(2)$ on $$ whose fixed points form a 2-dimensional submanifold $Δ⊂$ and which leaves $g$ invariant (see e.g. Ref. [ref] for an extended discussion). $Δ$ is called the rotation axis.

    An introduction to the theory of rotating relativistic stars · Stationary and axisymmetric spacetimes · 0.95

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