2010
DOI: 10.1134/s1063772910120012
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Formation of accretion disks in close-binary systems with magnetic fields

Abstract: We have developed a three-dimensional numerical model and applied it to simulate plasma flows in semi-detached binary systems whose accretor possesses a strong intrinsic magnetic field. The model is based on the assumption that the plasma dynamics are determined by the slow mean flow, which forms a backdrop for the rapid propagation of MHD waves. The equations describing the slow motion of matter were obtained by averaging over rapidly propagating pulsations. The numerical model includes the diffusion of magne… Show more

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Cited by 21 publications
(34 citation statements)
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References 37 publications
(65 reference statements)
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“…This code was used in [27,29,30] to investigate the flow structure in a close binary system (SS Cyg was taken as an example) with a relatively weak, purely dipolar magnetic field (10 5 G at the surface). A modification of the code was introduced in [31], which enables simulations of systems with strong dipolar magnetic fields (10 7 −10 8 G).…”
Section: Introductionmentioning
confidence: 99%
“…This code was used in [27,29,30] to investigate the flow structure in a close binary system (SS Cyg was taken as an example) with a relatively weak, purely dipolar magnetic field (10 5 G at the surface). A modification of the code was introduced in [31], which enables simulations of systems with strong dipolar magnetic fields (10 7 −10 8 G).…”
Section: Introductionmentioning
confidence: 99%
“…We run our binary wind simulation using the magnetohydrodynamics code Nurgush (Zhilkin & Bisikalo 2010). Nurgush solves the hydrodynamic equations in three dimensions using a non-inertial coordinate system that rotates with the orbital motion of the two stars.…”
Section: Methodsmentioning
confidence: 99%
“…To investigate how the value of the magnetic field influences the flow structure, we have performed calculations with various values of B a in a range from 10 5 to 10 8 G (Zhilkin & Bisikalo 2010c). Let us consider seven models, with values of the magnetic induction equal to: 10 5 G (model 1), 5 × 10 5 G (model 2), 10 6 G (model 3), 5 × 10 6 G (model 4), 10 7 G (model 5), 5 × 10 7 G (model 6), and 10 8 G (model 7).…”
Section: Changes In the Flow Structure With Increasing Of The Magnetimentioning
confidence: 99%
“…However, since the problem is very complicated, the investigations have been performed either in the frame of simplified models (King 1993;Wynn & King 1995;Wynn et al 1997;King & Wynn 1999;Norton et al 2004;Ikhsanov et al 2004;Norton et al 2008), or in a limited region of the stellar magnetosphere (Koldoba et al 2002;Romanova et al 2003Romanova et al , 2004aRomanova et al , 2004b. Only over the last few years, the authors have managed to develop a comprehensive 3D numerical model to calculate the flow structure in close binaries (Zhilkin & Bisikalo 2009, 2010a, 2010b, 2010c. In our approach, we use a complete system of MHD equations that allows one to describe all 510 D. V. Bisikalo & A. G. Zhilkin the main dynamic effects concerned with the magnetic field.…”
Section: Introductionmentioning
confidence: 99%