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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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The abstract, sentence by sentence
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.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| 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 |
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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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