Dynamo effect in unstirred self-gravitating turbulence

被引:6
作者
Brandenburg, Axel [1 ,2 ,3 ,4 ,5 ,6 ]
Ntormousi, Evangelia [7 ,8 ]
机构
[1] KTH Royal Inst Technol, Nordita, Hannes Alfvens Vag 12, SE-10691 Stockholm, Sweden
[2] Stockholm Univ, Hannes Alfvens Vag 12, SE-10691 Stockholm, Sweden
[3] Stockholm Univ, Dept Astron, Oskar Klein Ctr, AlbaNova, SE-10691 Stockholm, Sweden
[4] Carnegie Mellon Univ, McWilliams Ctr Cosmol, 5000 Forbes Ave, Pittsburgh, PA 15213 USA
[5] Carnegie Mellon Univ, Dept Phys, 5000 Forbes Ave, Pittsburgh, PA 15213 USA
[6] Ilia State Univ, Sch Nat Sci & Med, 3-5 Cholokashvili Ave, GE-0194 Tbilisi, Georgia
[7] Scuola Normale Super Pisa, Piazza Cavalieri 7, I-56126 Pisa, Italy
[8] Fdn Res & Technol Hellas, Inst Astrophys, GR-70013 Iraklion, Greece
基金
欧洲研究理事会; 瑞典研究理事会;
关键词
dynamo; ISM: general; (magnetohydrodynamics) MHD; turbulence; NONHELICAL HYDROMAGNETIC TURBULENCE; MAGNETIC-FIELD AMPLIFICATION; STAR-FORMATION; MOLECULAR CLOUDS; INTERSTELLAR-MEDIUM; COLLAPSE; SIMULATIONS; DRIVEN; MODEL; RESOLUTION;
D O I
10.1093/mnras/stac982
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
In many astrophysical environments, self-gravity can generate kinetic energy, which, in principle, is available for driving dynamo action. Using direct numerical simulations, we show that in unstirred self-gravitating subsonic turbulence with helicity and a magnetic Prandtl number of unity, there is a critical magnetic Reynolds number of about 25 above which the work done against the Lorentz force exceeds the Ohmic dissipation. The collapse itself drives predominantly irrotational motions that cannot be responsible for dynamo action. We find that, with a weak magnetic field, one-third of the work done by the gravitational force goes into compressional heating and the remaining two-thirds go first into kinetic energy of the turbulence before a fraction of it is converted further into magnetic and finally thermal energies. Close to the collapse, however, these fractions change toward 1/4 and 3/4 for compressional heating and kinetic energy, respectively. When the magnetic field is strong, the compressional heating fraction is unchanged. Out of the remaining kinetic energy, one quarter goes directly into magnetic energy via work against the Lorentz force. The fraction of vortical motions diminishes in favour of compressive motions that are almost exclusively driven by the Jeans instability. For an initially uniform magnetic field, field amplification at scales larger than those of the initial turbulence are driven by tangling.
引用
收藏
页码:2136 / 2151
页数:16
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