dc.contributor.author | Wurster, JH | |
dc.contributor.author | Bate, MR | |
dc.contributor.author | Price, DJ | |
dc.date.accessioned | 2018-03-20T14:01:41Z | |
dc.date.issued | 2018-02-14 | |
dc.description.abstract | What cosmic ray ionization rate is required such that a non-ideal magnetohydrodynamics (MHD) simulation of a collapsing molecular cloud will follow the same evolutionary path as an ideal MHD simulation or as a purely hydrodynamics simulation? To investigate this question, we perform three-dimensional smoothed particle non-ideal MHD simulations of the gravitational collapse of rotating, one solar mass, magnetized molecular cloud cores, which include Ohmic resistivity, ambipolar diffusion, and the Hall effect. We assume a uniform grain size of ag = 0.1 μm, and our free parameter is the cosmic ray ionization rate, ζcr. We evolve our models, where possible, until they have produced a first hydrostatic core. Models with ζcr ≳ 10−13 s−1 are indistinguishable from ideal MHD models, and the evolution of the model with ζcr = 10−14 s−1 matches the evolution of the ideal MHD model within 1 per cent when considering maximum density, magnetic energy, and maximum magnetic field strength as a function of time; these results are independent of ag. Models with very low ionization rates (ζcr ≲ 10−24 s−1) are required to approach hydrodynamical collapse, and even lower ionization rates may be required for larger ag. Thus, it is possible to reproduce ideal MHD and purely hydrodynamical collapses using non-ideal MHD given an appropriate cosmic ray ionization rate. However, realistic cosmic ray ionization rates approach neither limit; thus, non-ideal MHD cannot be neglected in star formation simulations. | en_GB |
dc.description.sponsorship | JW and MRB acknowledge support from the European Research Council under the European Community's Seventh Framework Programme (FP7/2007- 2013 grant agreement no. 339248). DJP received funding via Australian Research Council grants FT130100034, DP130102078, and DP180104235. This work was supported by resources on the swinSTAR national facility at Swinburne University of Technology. swinSTAR is funded by Swinburne and the Australian Government's Education Investment Fund. | en_GB |
dc.identifier.citation | Vol. 476 (2), pp. 2063 - 2074 | en_GB |
dc.identifier.doi | 10.1093/mnras/sty392 | |
dc.identifier.uri | http://hdl.handle.net/10871/32176 | |
dc.language.iso | en | en_GB |
dc.publisher | Oxford University Press (OUP) / Royal Astronomical Society | en_GB |
dc.relation.url | https://doi.org/10.24378/exe.263 | en_GB |
dc.rights | © 2018 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society. All rights reserved. | en_GB |
dc.subject | magnetic fields | en_GB |
dc.subject | MHD | en_GB |
dc.subject | methods: numerical | en_GB |
dc.subject | stars: formation | en_GB |
dc.title | The effect of extreme ionization rates during the initial collapse of a molecular cloud core (article) | en_GB |
dc.type | Article | en_GB |
dc.date.available | 2018-03-20T14:01:41Z | |
dc.identifier.issn | 0035-8711 | |
dc.description | This is the final version of the article. Available from OUP via the DOI in this record. | en_GB |
dc.description | The dataset associated with this article is located in ORE at: https://doi.org/10.24378/exe.263 | en_GB |
dc.identifier.journal | Monthly Notices of the Royal Astronomical Society | en_GB |