859 research outputs found

    Asymptotic models of meridional flows in thin viscous accretion disks

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    We present the results of numerical integrations yielding the structure of and meridional flow in axisymmetric thin viscous accretion disk models. The solutions are obtained by simplifying and approximating first the equations, using systematic asymptotic expansions in the small parameter ϵ\epsilon, measuring the relative disk thickness. The vertical structure is solved including radiative transfer in the diffusion approximation. Carrying out the expansion to second order in ϵ\epsilon we obtain, for low enough values of the viscosity parameter α\alpha, solutions containing {\em backflows}. These solutions are similar to the results first found by Urpin (1984), who used approximations that are only valid for large radii and the asymptotic analytical solutions of Klu\'zniak & Kita (1997), valid only for polytropic disks. Our results may be important for several outstanding issues in accretion disk theory.Comment: 5 figure

    A weakly nonlinear analysis of the magnetorotational instability in a model channel flow

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    We show by means of a perturbative weakly nonlinear analysis that the axisymmetric magnetorotational instability (MRI) of a viscous, resistive, incompressible rotating shear flow in a thin channel gives rise to a real Ginzburg-Landau equation for the disturbance amplitude. For small magnetic Prandtl number (Pm{\cal P}_{\rm m}), the saturation amplitude is Pm\propto \sqrt{{\cal P}_{\rm m}} and the resulting momentum transport scales as R1{\cal R}^{-1}, where R\cal R is the {\em hydrodynamic} Reynolds number. Simplifying assumptions, such as linear shear base flow, mathematically expedient boundary conditions and continuous spectrum of the vertical linear modes, are used to facilitate this analysis. The asymptotic results are shown to comply with numerical calculations using a spectral code. They suggest that the transport due to the nonlinearly developed MRI may be very small in experimental setups with Pm1{\cal P}_{\rm m} \ll 1.Comment: Accepted to Physical Review Letters - Nov. 30, 2006. In final for

    Grover's search with faults on some marked elements

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    Grover's algorithm is a quantum query algorithm solving the unstructured search problem of size NN using O(N)O(\sqrt{N}) queries. It provides a significant speed-up over any classical algorithm \cite{Gro96}. The running time of the algorithm, however, is very sensitive to errors in queries. It is known that if query may fail (report all marked elements as unmarked) the algorithm needs Ω(N)\Omega(N) queries to find a marked element \cite{RS08}. \cite{AB+13} have proved the same result for the model where each marked element has its own probability to be reported as unmarked. We study the behavior of Grover's algorithm in the model where the search space contains both faulty and non-faulty marked elements. We show that in this setting it is indeed possible to find one of non-faulty marked items in O(N)O(\sqrt{N}) queries. We also analyze the limiting behavior of the algorithm for a large number of steps and show the existence and the structure of limiting state ρlim\rho_{lim}.Comment: 17 pages, 6 figure

    Non-exponential hydrodynamical growth in density-stratified thin Keplerian discs

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    The short time evolution of three dimensional small perturbations is studied. Exhibiting spectral asymptotic stability, thin discs are nonetheless shown to host intensive hydrodynamical activity in the shape of non modal growth of initial small perturbations. Two mechanisms that lead to such behavior are identified and studied, namely, non-resonant excitation of vertically confined sound waves by stable planar inertia-coriolis modes that results in linear growth with time, as well as resonant coupling of those two modes that leads to a quadratic growth of the initial perturbations. It is further speculated that the non modal growth can give rise to secondary strato-rotational instabilities and thus lead to a new route to turbulence generation in thin discs

    Revised research about chaotic dynamics in Manko et al. spacetime

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    A recent work by Dubeibe et al. [Phys. Rev. D 75, 023008 (2007)] stated that chaos phenomenon of test particles in gravitational field of rotating neutron stars which are described by Manko, Sanabria-Gomez, and Manko (Manko et al.) metric can only occur when the stars have oblate deformation. But the chaotic motions they found are limited in a very narrow zone which is very close to the center of the massive bodies. This paper argues that this is impossible because the region is actually inside of the stars, so the motions cannot exist at this place. In this paper, we scan all parameters space and find chaos and unstable fixed points outside of stars with big mass-quadrupole moments. The calculations show that chaos can only occur when the stars have prolate deformation. Because real deformation of stars should be oblate, all orbits of test particles around the rotating neutron stars described by Manko et al. solutions are regular. The case of nonzero dipolar magnetic moment has also been taken into account in this study.Comment: 6 pages, 5 figure

    Hydrodynamic response of rotationally supported flows in the Small Shearing Box model

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    The hydrodynamic response of the inviscid small shearing box model of a midplane section of a rotationally supported astrophysical disk is examined. An energy functional E{\cal E} is formulated for the general nonlinear problem. It is found that the fate of disturbances is related to the conservation of this quantity which, in turn, depends on the boundary conditions utilized: E{\cal E} is conserved for channel boundary conditions while it is not conserved in general for shearing box conditions. Linearized disturbances subject to channel boundary conditions have normal-modes described by Bessel Functions and are qualitatively governed by a quantity Σ\Sigma which is a measure of the ratio between the azimuthal and vertical wavelengths. Inertial oscillations ensue if Σ>1\Sigma >1 - otherwise disturbances must in general be treated as an initial value problem. We reflect upon these results and offer a speculation.Comment: 6 pages, resubmitted to Astronomy and Astrophysics, shortened with references adde
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