2001
DOI: 10.1086/323631
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Magnetic Helix Formation Driven by Keplerian Disk Rotation in an External Plasma Pressure: The Initial Expansion Stage

Abstract: We study the evolution of a magnetic arcade that is anchored to an accretion disk and is sheared by the di †erential rotation of a Keplerian disk. By including an extremely low external plasma pressure at large distances, we obtain a sequence of axisymmetric magnetostatic equilibria and show that there is a fundamental di †erence between Ðeld lines that are a †ected by the plasma pressure and those that are not (i.e., force free). Force-free Ðelds, while being twisted by the di †erential rotation of the disk, … Show more

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Cited by 51 publications
(79 citation statements)
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“…Choudhuri & Konigl 1986). Secondly, it is probable that jets are electromagnetically dominated on parsec scales (Lynden-Bell 1996Ustyugova et al 2000;Li et al 2001;Lovelace et al 2002;; see also Section 6), so that their structure is determined by relativistic force-free electrodynamics. In this work, we assume that the jets are strongly magnetized and are described by relativistic force-free electrodynamics.…”
Section: E M I S S I O N F Ro M ' F I L L E D ' J E T Smentioning
confidence: 99%
“…Choudhuri & Konigl 1986). Secondly, it is probable that jets are electromagnetically dominated on parsec scales (Lynden-Bell 1996Ustyugova et al 2000;Li et al 2001;Lovelace et al 2002;; see also Section 6), so that their structure is determined by relativistic force-free electrodynamics. In this work, we assume that the jets are strongly magnetized and are described by relativistic force-free electrodynamics.…”
Section: E M I S S I O N F Ro M ' F I L L E D ' J E T Smentioning
confidence: 99%
“…Here, we consider further the theory of Poynting outflows (Li et al 2001). We assume that magnetic field loops thread a differentially rotating, highly conducting Keplerian accretion disk at some initial time t ¼ 0.…”
Section: Theory Of Poynting Outflowsmentioning
confidence: 99%
“…with D à @ 2 =@r 2 À ð1=rÞð@=@rÞ þ @ 2 =@z 2 ; which is the GS equation for É (see, e.g., Lovelace et al 1987;Li et al 2001). Ampère's law gives H dl x B ¼ ð4=cÞ R dS x J, so that rB ðr; zÞ ¼ HðÉÞ is ð2=cÞ times the current flowing through a circular area of radius r (with normalẑ z) labeled by Éðr; zÞ ¼ const.…”
Section: Theory Of Poynting Outflowsmentioning
confidence: 99%
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