Plasma Confinement by Direct-Current Magnetic Fields Assisted by an Arbitrary External Force

1962 ◽  
Vol 5 (6) ◽  
pp. 730 ◽  
Author(s):  
D. G. Dow
1997 ◽  
Author(s):  
John W. Obringer ◽  
Tara E. Nolan ◽  
Brandon Horne ◽  
Brian Kelchner

2021 ◽  
Author(s):  
Luana Albert ◽  
Frédéric Olivier ◽  
Aurélie Jolivet ◽  
Laurent Chauvaud ◽  
Sylvain Chauvaud

Author(s):  
R. S. MacKay

Stokes’ theorem, in its original form and Cartan’s generalization, is crucial for designing magnetic fields to confine plasma (ionized gas). The paper illustrates its use, in particular to address the question whether quasi-symmetric fields, those for which guiding-centre motion is integrable, can be made with little or no toroidal current. This article is part of the theme issue ‘Stokes at 200 (Part 1)’.


2021 ◽  
Vol 922 (1) ◽  
pp. 63
Author(s):  
Shuhei Kashiwamura ◽  
Yutaka Ohira

Abstract We present new-generation mechanisms of magnetic fields in supernova remnant shocks propagating to partially ionized plasmas in the early universe. Upstream plasmas are dissipated at the collisionless shock, but hydrogen atoms are not dissipated because they do not interact with electromagnetic fields. After the hydrogen atoms are ionized in the shock downstream region, they become cold proton beams that induce the electron return current. The injection of the beam protons can be interpreted as an external force acting on the downstream proton plasma. We show that the effective external force and the electron return current can generate magnetic fields without any seed magnetic fields. The magnetic field strength is estimated to be B ∼ 10 − 14 – 10 − 11 G , where the characteristic length scale is the mean free path of charge exchange, ∼ 10 15 cm . Since protons are marginally magnetized by the generated magnetic field in the downstream region, the magnetic field could be amplified to larger values and stretched to larger scales by turbulent dynamo and expansion.


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