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dc.contributor.authorWurster, J.
dc.contributor.authorBate, Matthew R
dc.contributor.authorPrice, Daniel J
dc.date.accessioned2019-10-25T09:30:03Z
dc.date.available2019-10-25T09:30:03Z
dc.date.issued2018-05
dc.identifier.citationWurster , J , Bate , M R & Price , D J 2018 , ' The effect of extreme ionization rates during the initial collapse of a molecular cloud core ' , Monthly Notices of the Royal Astronomical Society , vol. 476 , no. 2 , pp. 2063-2074 . https://doi.org/10.1093/mnras/sty392en
dc.identifier.issn0035-8711
dc.identifier.otherPURE: 262150134
dc.identifier.otherPURE UUID: c9d36e7d-2c63-4e14-b8e8-4ddcaba7a373
dc.identifier.otherBibtex: WursterBatePrice2018ion
dc.identifier.otherScopus: 85055146330
dc.identifier.otherORCID: /0000-0003-0688-5332/work/63716923
dc.identifier.urihttps://hdl.handle.net/10023/18764
dc.description.abstractWhat 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.
dc.format.extent12
dc.language.isoeng
dc.relation.ispartofMonthly Notices of the Royal Astronomical Societyen
dc.rights© Copyright 2018 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society. This work has been made available online in accordance with publisher policies or with permission. Permission for further reuse of this content should be sought from the publisher or the rights holder. This is the final published version of the work, which was originally published at https://doi.org/10.1093/mnras/sty392en
dc.subjectMagnetic fieldsen
dc.subjectMHDen
dc.subjectMethods: numericalen
dc.subjectStars: formationen
dc.subjectQB Astronomyen
dc.subjectQC Physicsen
dc.subjectT-NDASen
dc.subject.lccQBen
dc.subject.lccQCen
dc.titleThe effect of extreme ionization rates during the initial collapse of a molecular cloud coreen
dc.typeJournal articleen
dc.description.versionPublisher PDFen
dc.contributor.institutionUniversity of St Andrews. School of Physics and Astronomyen
dc.identifier.doihttps://doi.org/10.1093/mnras/sty392
dc.description.statusPeer revieweden
dc.identifier.urlhttps://arxiv.org/abs/1802.04872en


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