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On the Perturbations of Viscous Rotating Newtonian Fluids

Astrophysics · Submitted 22 Feb 2000

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

The authors' main claim In this case, we find that viscosity causes the fundamental p- and g- modes to grow while the fundamental c-mode could have either sign of the damping rate.

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arXiv IDastro-ph/0002419 (version 1)
Pith ID6FCOZO54, Pith's permanent record of this paper and its review
CitationManuel Ortega-Rodriguez, Robert V. Wagoner. "On the Perturbations of Viscous Rotating Newtonian Fluids." arXiv:astro-ph/0002419 (2000). https://pith.science/paper/6FCOZO54
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Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-23: 1 request, 5,590 input tokens.

What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.92 · human participants 0.01 · controlled comparison 0.53 · randomized assignment 0.01 · states quantitative result 0.09 · compares with prior results 0.87 · mentions code or data availability 0.02.

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arXiv listing abstract v1. Results and the main claim are underlined; .

The perturbations of weakly-viscous, barotropic, non-self-gravitating, Newtonian rotating fluids are analyzed via a single partial differential equation. The results are then used to find an expression for the viscosity-induced normal-mode complex eigenfrequency shift, with respect to the case of adiabatic perturbations. However, the effects of viscosity are assumed to have been incorporated in the unperturbed (equilibrium) model. This paper is an extension of the normal-mode formalism developed by Ipser & Lindblom for adiabatic pulsations of purely-rotating perfect fluids. The formulas derived are readily applicable to the perturbations of thin and thick accretion disks. We provide explicit expressions for thin disks, employing results from previous relativistic analyses of adiabatic normal modes of oscillation. In this case, we find that viscosity causes the fundamental p- and g- modes to grow while the fundamental c-mode could have either sign of the damping rate.

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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 The perturbations of weakly-viscous, barotropic, non-self-gravitating, Newtonian rotating fluids are analyzed via a single partial differential equation. contribution 0.67 0.91 0.11 asserted 1.00
s1 The results are then used to find an expression for the viscosity-induced normal-mode complex eigenfrequency shift, with respect to the case of adiabatic perturbations. result 0.79 0.93 0.25 asserted 1.00
s2 However, the effects of viscosity are assumed to have been incorporated in the unperturbed (equilibrium) model. limitation 0.96 0.30 0.04 asserted 0.97
s3 This paper is an extension of the normal-mode formalism developed by Ipser & Lindblom for adiabatic pulsations of purely-rotating perfect fluids. background 0.77 0.39 0.05 asserted 1.00
s4 The formulas derived are readily applicable to the perturbations of thin and thick accretion disks. contribution 0.44 0.55 0.08 asserted 0.94
s5 We provide explicit expressions for thin disks, employing results from previous relativistic analyses of adiabatic normal modes of oscillation. contribution 0.74 0.85 0.06 asserted 1.00
s6 In this case, we find that viscosity causes the fundamental p- and g- modes to grow while the fundamental c-mode could have either sign of the damping rate. result 1.00 0.93 0.47 hedged possibility 0.70

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

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Original abstract

The perturbations of weakly-viscous, barotropic, non-self-gravitating, Newtonian rotating fluids are analyzed via a single partial differential equation. The results are then used to find an expression for the viscosity-induced normal-mode complex eigenfrequency shift, with respect to the case of adiabatic perturbations. However, the effects of viscosity are assumed to have been incorporated in the unperturbed (equilibrium) model. This paper is an extension of the normal-mode formalism developed by Ipser & Lindblom for adiabatic pulsations of purely-rotating perfect fluids. The formulas derived are readily applicable to the perturbations of thin and thick accretion disks. We provide explicit expressions for thin disks, employing results from previous relativistic analyses of adiabatic normal modes of oscillation. In this case, we find that viscosity causes the fundamental p- and g- modes to grow while the fundamental c-mode could have either sign of the damping rate.

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