dc.contributor.author | Carlyle, J | |
dc.contributor.author | Hillier, AS | |
dc.date.accessioned | 2017-09-01T11:34:34Z | |
dc.date.issued | 2017-07-25 | |
dc.description.abstract | This work examines the effect of the embedded magnetic field strength on the non-linear development of the magnetic Rayleigh-Taylor Instability (RTI) (with a field-aligned interface) in an ideal gas close to the incompressible limit in three dimensions. Numerical experiments are conducted in a domain sufficiently large so as to allow the predicted critical modes to develop in a physically realistic manner. The ratio between gravity, which drives the instability in this case (as well as in several of the corresponding observations), and magnetic field strength is taken up to a ratio which accurately reflects that of observed astrophysical plasma, in order to allow comparison between the results of the simulations and the observational data which served as inspiration for this work. This study finds reduced non-linear growth of the rising bubbles of the RTI for stronger magnetic fields, and that this is directly due to the change in magnetic field strength, rather than the indirect effect of altering characteristic length scales with respect to domain size. By examining the growth of the falling spikes, the growth rate appears to be enhanced for the strongest magnetic field strengths, suggesting that rather than affecting the development of the system as a whole, increased magnetic field strengths in fact introduce an asymmetry to the system. Further investigation of this effect also revealed that the greater this asymmetry, the less efficiently the gravitational energy is released. By better understanding the under-studied regime of such a major phenomenon in astrophysics, deeper explanations for observations may be sought, and this work illustrates that the strength of magnetic fields in astrophysical
plasmas influences observed RTI in subtle and complex ways. | en_GB |
dc.description.sponsorship | Jack Carlyle conducted this work during a PhD joint-funded by University College London and The Max Planck Institute for Solar System Research, as well as whilst receiving funding as a Research Fellow from the European Space Agency. Andrew Hillier is supported by his STFC Emest Rutherford Fellowship grant number ST/L00397X/2. | en_GB |
dc.identifier.citation | Published online 25 July 2017 | en_GB |
dc.identifier.doi | 10.1051/0004-6361/201730802 | |
dc.identifier.uri | http://hdl.handle.net/10871/29160 | |
dc.language.iso | en | en_GB |
dc.publisher | EDP Sciences for European Southern Observatory (ESO) | en_GB |
dc.subject | Instabilities | en_GB |
dc.subject | Magnetohydrodynamics (MHD) | en_GB |
dc.subject | Plasmas | en_GB |
dc.subject | Magnetic fields | en_GB |
dc.title | The Non-Linear Growth of the Magnetic Rayleigh-Taylor Instability | en_GB |
dc.type | Article | en_GB |
dc.date.available | 2017-09-01T11:34:34Z | |
dc.identifier.issn | 0004-6361 | |
dc.description | This is the author accepted manuscript. The final version is available from EDP Sciences via the DOI in this record. | en_GB |
dc.identifier.journal | Astronomy and Astrophysics | en_GB |