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dc.contributor.authorWurster, James
dc.contributor.authorBate, Matthew
dc.date.accessioned2019-08-28T09:02:58Z
dc.date.issued2019-08-28
dc.date.updated2019-08-28T03:28:56Z
dc.description.abstractWe investigate the formation and fragmentation of discs using a suite of three-dimensional smoothed particle radiative magnetohydrodynamics simulations. Our models are initialised as 1 solar mass rotating Bonnor-Ebert spheres that are threaded with a uniform magnetic field. We examine the effect of including ideal and non-ideal magnetic fields, the orientation and strength of the magnetic field, and the initial rotational rate. We follow the gravitational collapse and early evolution of each system until the final classification of the protostellar disc can be determined. Of our 105 models, 41 fragment, 21 form a spiral structure but do not fragment, and another 12 form smooth discs. Fragmentation is more likely to occur for faster initial rotation rates and weaker magnetic fields. For stronger magnetic field strengths, the inclusion of non-ideal MHD promotes disc formation, and several of these models fragment, whereas their ideal MHD counterparts do not. For the models that fragment, there is no correlation between our parameters and where or when the fragmentation occurs. Bipolar outflows are launched in only 17 models, and these models have strong magnetic fields that are initially parallel to the rotation axis. Counter-rotating envelopes form in four slowly-rotating, strong-field models – including one ideal MHD model – indicating they form only in a small fraction of the parameter space investigated.en_GB
dc.description.sponsorshipEuropean Research Council (ERC)en_GB
dc.description.sponsorshipScience and Technology Facilities Council (STFC)en_GB
dc.description.sponsorshipScience and Technology Facilities Council (STFC)en_GB
dc.description.sponsorshipScience and Technology Facilities Council (STFC)en_GB
dc.description.sponsorshipScience and Technology Facilities Council (STFC)en_GB
dc.description.sponsorshipScience and Technology Facilities Council (STFC)en_GB
dc.identifier.doi10.24378/exe.1743
dc.identifier.grantnumberFP7/2007- 2013 grant agreement no. 339248en_GB
dc.identifier.grantnumberST/K000373/1en_GB
dc.identifier.grantnumberST/K0003259/1en_GB
dc.identifier.grantnumberST/K000373/1en_GB
dc.identifier.grantnumberST/R002363/1en_GB
dc.identifier.grantnumberST/R001014/1en_GB
dc.identifier.urihttp://hdl.handle.net/10871/38469
dc.language.isoenen_GB
dc.publisherUniversity of Exeteren_GB
dc.relation.urlhttp://hdl.handle.net/10871/37605en_GB
dc.rightsCC BY 4.0en_GB
dc.subjectmethods: numericalen_GB
dc.subjectMHDen_GB
dc.subjectmagnetic fieldsen_GB
dc.subjectstars: formationen_GB
dc.subjectplanets and satellites: formationen_GB
dc.subjectaccretion: accretion discsen_GB
dc.titleDisc formation and fragmentation using radiative non-ideal magnetohydrodynamics (dataset)en_GB
dc.typeDataseten_GB
dc.date.available2019-08-28T09:02:58Z
dc.descriptionThis is the data created for Wurster & Bate (2019): Disc formation and fragmentation using radiative non-ideal magnetohydrodynamics. This dataset was created using the smoothed particle magnetohydrodynamics code sphNG, which included v1.2.1 of the NICIL library (Wurster 2016) to calculate the non-ideal MHD coefficients. The raw data and important files have been uploaded; the data files can be read with either sphNG (proprietary SPH code), or with the public graphics programme Splash (Price 2007). Each model has been tarred in its own file, where the model name is the file name. For the hydrodynamic models, the names are HObb.tar.gz, where bb is 100 times the initial rotation in terms of the orbital radius. For the magnetised models, the names are aObbMuccBdd.tar.gz, where a=I (N) for ideal (non-ideal) MHD, bb is as above, cc is the normalised mass-to-flux ratio, and dd the magnetic field direction (xn for -B_x, zn for -B_z, zp for +B_z). 01_Misc.tar.gz contains some useful analysis routines and lists; 02_Images.tar.gz includes the images and code required for the figures in the manuscript, and addition figures and code that were used in the analysis. Due to high time resolution of some models, several intermediate/redundant dump files were deleted during production to save space; thus the dump numbers are not sequential in these .tar.gz files, and the missing number represent the deleted dump files.en_GB
dc.descriptionThe article associated with this dataset is located in ORE at: http://hdl.handle.net/10871/37605en_GB
dc.rights.urihttps://creativecommons.org/licenses/by/4.0en_GB
rioxxterms.versionNAen_GB
rioxxterms.typeOtheren_GB
refterms.dateFOA2019-08-28T09:03:03Z


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