Dissipation of magnetic fields in very dense interstellar clouds – I. Formulation and conditions for efficient dissipation

The drift velocity VB of magnetic fields relative to the fluid is obtained by solving the motions of many kinds of charged particles. Any closed curve moving with vB has a constant magnetic flux. This velocity contains the effects of both plasma drift and Joule dissipation. At the hydrogen density $...

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Bibliographic Details
Published in:Monthly notices of the Royal Astronomical Society Vol. 218; no. 4; pp. 663 - 684
Main Authors: Nakano, Takenori, Umebayashi, Toyoharu
Format: Journal Article
Language:English
Published: Oxford, UK Oxford University Press 01-02-1986
Blackwell Science
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Summary:The drift velocity VB of magnetic fields relative to the fluid is obtained by solving the motions of many kinds of charged particles. Any closed curve moving with vB has a constant magnetic flux. This velocity contains the effects of both plasma drift and Joule dissipation. At the hydrogen density ${n}_\text{H}\gtrsim{10}^{11}\,\text{cm}^{-3}$, υB is at least 10 times smaller than the free-fall velocity uf, and then field dissipation is inefficient. At ${n}^{H}\gtrsim{10}^{12}\,\text{cm}^{-3}$ and temperature $T\lt{10}^{3}\,\text{K}$ where thermal ionization is inefficient, however, υB exceeds uf unless the characteristic curvature radius of field lines is much greater than the characteristic length of the cloud. In such a situation, charged grains are more abundant than ions, and the field decays mainly through Joule dissipation. Thus the magnetic field is decoupled from the gas and only nearly current-free fields can exist in a part of the cloud with ${n}_\text{H}\gtrsim{10}^{12}\,\text{cm}^{-3}\,\text{and}\,\,T\lt{10}^{3}\,\text{K}$.
Bibliography:istex:F709C171C67407A5001695AF7B0A89F304257781
ark:/67375/HXZ-7ZV9P65Z-R
ISSN:0035-8711
1365-2966
DOI:10.1093/mnras/218.4.663