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Magnetohydrodynamics of Cloud Collisions in a Multiphase Interstellar Medium
Author(s) -
Francesco Miniati,
Dongsu Ryu,
Andrea Ferrara,
T. W. Jones
Publication year - 1999
Publication title -
the astrophysical journal
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.376
H-Index - 489
eISSN - 1538-4357
pISSN - 0004-637X
DOI - 10.1086/306599
Subject(s) - physics , radiative transfer , magnetohydrodynamics , magnetic field , interstellar medium , molecular cloud , interstellar cloud , adiabatic process , astrophysics , computational physics , stars , galaxy , quantum mechanics , thermodynamics
We extend previous studies of the physics of interstellar cloud collisions bybeginning investigation of the role of magnetic fields through 2Dmagnetohydrodynamic (MHD) numerical simulations. We study head-on collisionsbetween equal mass, mildly supersonic diffuse clouds. We include a moderatemagnetic field and two limiting field geometries, with the field lines parallel(aligned) and perpendicular (transverse) to the colliding cloud motion. Weexplore both adiabatic and radiative cases, as well as symmetric and asymmetricones. We also compute collisions between clouds evolved through prior motion inthe intercloud medium and compare with unevolved cases. We find that: In the (i) aligned case, adiabatic collisions, like their HDcounterparts, are very disruptive, independent of the cloud symmetry. However,when radiative processes are taken into account, partial coalescence takesplace even in the asymmetric case, unlike the HD calculations. In the (ii)transverse case, collisions between initially adjacent unevolved clouds arealmost unaffected by magnetic fields. However, the interaction with themagnetized intercloud gas during the pre-collision evolution produces a regionof very high magnetic energy in front of the cloud. In collisions betweenevolved clouds with transverse field geometry, this region acts like a``bumper'', preventing direct contact between the clouds, and eventuallyreverses their motion. The ``elasticity'', defined as the ratio of the final tothe initial kinetic energy of each cloud, is about 0.5-0.6 in the cases weconsidered. This behavior is found both in adiabatic and radiative cases.

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