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 $...
Saved in:
Published in: | Monthly notices of the Royal Astronomical Society Vol. 218; no. 4; pp. 663 - 684 |
---|---|
Main Authors: | , |
Format: | Journal Article |
Language: | English |
Published: |
Oxford, UK
Oxford University Press
01-02-1986
Blackwell Science |
Subjects: | |
Online Access: | Get full text |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
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 |