2015
DOI: 10.1093/mnras/stv2466
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The effect of large-scale magnetic field on outflow in ADAFs: an odd symmetry configuration

Abstract: We construct self-similar inflow-outflow solutions for a hot viscous-resistive accretion flow with large scale magnetic fields that have odd symmetry with respect to the equatorial plane in B θ , and even symmetry in B r and B φ . Following previous authors, we also assume that the polar velocity v θ is nonzero. We focus on four parameters: β r0 , β φ0 (the plasma beta parameters for associated with magnetic field components at the equatorial plane), the magnetic resistivity η 0 , and the density index n = −d … Show more

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Cited by 21 publications
(29 citation statements)
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References 61 publications
(58 reference statements)
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“…The magnetic field plays a crucial role in the dynamical structure and the observational properties of accretion disc. Kaburaki (2000), Abbassi et al (2010 ), Ghasemnezhad et al(2012), , Samadi & Abbassi (2016), and Samadi et al (2014) studied the effect of magnetic field on hot accretion flow (ADAF) in the recent years. But the magnetized slim disc model has been less studied.…”
Section: Introductionmentioning
confidence: 99%
“…The magnetic field plays a crucial role in the dynamical structure and the observational properties of accretion disc. Kaburaki (2000), Abbassi et al (2010 ), Ghasemnezhad et al(2012), , Samadi & Abbassi (2016), and Samadi et al (2014) studied the effect of magnetic field on hot accretion flow (ADAF) in the recent years. But the magnetized slim disc model has been less studied.…”
Section: Introductionmentioning
confidence: 99%
“…In the one-dimensional works, the existence of wind is often an assumption (e.g. Blandford & Begelman 1999;Akizuki & Fukue 2006;Abbassi et al 2008;Zhang & Dai 2008;Bu et al 2009 Mosallanezhad et al 2014;Gu 2015;Samadi & Abbassi 2016 ) but not all (e.g., Narayan & Yi 1995 and references therein). In all these works magnetic field is not included.…”
Section: Introductionmentioning
confidence: 99%
“…Figure 6 displays isodensity contours for the asymmetric configuration of disk which is caused by asymmetric poloidal magnetic field. In the reflection symmetry of quantities, isodensity contours usually make close shapes such as Fig.2 of Samadi et al (2016). But here, non-zero B r in the mid-plane makes isodensity contour to be different in upper and lower sides of the disk.…”
Section: Vertical Structurementioning
confidence: 95%
“…the above equation is the result of ∂B r /∂t = 0 and ∂B θ /∂t = 0 (for more details refer to Samadi & Abbassi 2016). To satisfy ∇ · B = 0 we can express the poloidal magnetic field in terms of a flux function ψ(r, θ) (Lovelace et al 1987),…”
Section: Equationsmentioning
confidence: 99%
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