Quasi-viscous accretion flow -- I: Equilibrium conditions and asymptotic behaviour
arXiv:0812.4793 · doi:10.1111/j.1365-2966.2009.14977.x
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 -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 Schrödinger'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.
15 pages
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- On Spin Dependence of Relativistic Acoustic Geometry
- Axially Symmetric Accretion of Fractal Medium onto Rotating Black Holes and the emergence of the Acoustic Manifold
- Nonlinear variations in axisymmetric accretion
- Carter-Penrose diagrams for emergent spacetime in axisymmetrically accreting black hole systems
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- Dissipation and acoustic tunnelling about the sonic horizon of Bondi accretion
- Transonicity in black hole accretion -- A mathematical study using the generalized Sturm chains