# Quasi-viscous accretion flow -- I: Equilibrium conditions and asymptotic behaviour

Source: [Quasi-viscous accretion flow -- I: Equilibrium conditions and asymptotic behaviour](<https://www.sota2.com/research/paper/68fa2eef1e209131ce867778>)

Collection index: [llms.txt](<https://www.sota2.com/research/llms.txt>)

Data updated: 2025-10-28T13:53:30.913Z

Authors: Jayanta K. Bhattacharjee, Atri Bhattacharya, Tapas K. Das, Arnab K. Ray

Published: 2008-12-28T05:10:56.000Z

## Abstract

In a novel approach to studying viscous accretion flows, viscosity has been introduced as a perturbative effect, involving a first-order correction in the $\\alpha$-viscosity parameter. This method reduces the problem of solving a second-order nonlinear differential equation (Navier-Stokes equation) to that of an effective first-order equation. Viscosity breaks down the invariance of the equilibrium conditions for stationary inflow and outflow solutions, and distinguishes accretion from wind. Under a dynamical systems classification, the only feasible critical points of this "quasi-viscous" flow are saddle points and spirals. A linearised and radially propagating time-dependent perturbation gives rise to secular instability on large spatial scales of the disc. Further, on these same length scales, the velocity evolution equation of the quasi-viscous flow has been transformed to bear a formal closeness with Schr\\"odinger's equation with a repulsive potential. Compatible with the transport of angular momentum to the outer regions of the disc, a viscosity-limited length scale has been defined for the full spatial extent over which the accretion process would be viable.

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## Original sources and implementation

[Original paper](<https://arxiv.org/abs/0812.4793>)

[PDF](<https://arxiv.org/pdf/0812.4793.pdf>)
