TITLE: Collapse and Fragmentation of Magnetic Molecular Cloud Cores with the Enzo AMR MHD Code. I. Uniform Density Spheres
AUTHORS: Alan P. Boss & Sandra A. Keiser
AUTHORS’ INSTITUTION: Department of Terrestrial Magnetism, Carnegie Institution for Science
- Adaptive Mesh Refinement (AMR): The length scales required to model star formation span many orders of magnitude. Giant molecular clouds are measured on parsec scales (1 pc ~ 3 x 1013 km) whereas the radius of the sun is ~ 7 x 105 km. So modeling the collapse of a molecular cloud all the way to star formation requires a code which can span 8 orders of magnitude! AMR works by starting with a coarse grid, and inserting new grid points points when they are needed to trace small scale physics, and removing the grid points when they are no longer needed. This cuts down on memory usage and computing time.
- Magnetohydrodynamics is a combination of fluid dynamics (hydro-) and electricity and magnetism (magneto-). A molecular cloud is a fluid which can be described by the Navier-Stokes Equations. This set of equations traces how energy, momentum, and mass is conserved in a fluid in terms of thermodynamic quantities such as pressure, temperature, and density, as well as the velocity of the material. Furthermore, magnetohydrodynamics invokes Maxwell’s Equations to trace the interplay of currents and magnetic fields in a conductive fluid.
Enzo 2.0 is overrun with complicated physics. As a result, this code can model many complicated processes, but it is crucial to first verify that the code can reproduce known results with simpler physics. Boss & Keiser go about this self-check by testing the code on a classical star formation case: the collapse of a non-magnetic, isothermal cloud model. Many researchers have verified that when a large density perturbation (50%) is introduced into a 1 solar mass cloud, the material collapses into not just one star, but a binary system. Boss & Keiser reproduce this result, thus they can proceed to the magnetic case.
The star formation simulations presented in this paper utilize simple initial conditions for the cloud (e.g. spherical, uniform density), but still require multiple inputs to test the potential effects of magnetic fields. First, the models require an equation of state, or a relation between the state variables of the cloud such as pressure and density. Boss & Keiser examine both the simple isothermal case where P ∝ p and a barotropic equation of state where P ∝ p7/5 at high densities (e.g. Price & Bate, 2007). The models also require inputs related to the magnetic field. In these simulations, the magnetic fields were given an initial strength and then “frozen in” such that they didn’t vary with time, and the initial orientation of the field was set to be either parallel or perpendicular to the rotation axis of the cloud. By computing a large number of models with these relatively simple inputs, Boss & Keiser were able to determine 3 possible outcomes for molecular clouds with strong magnetic fields:
- The cloud begins to collapse, and increases significantly in density; however, the magnetic fields prevents complete collapse of the cloud, thus it doesn’t form stars.
- The cloud collapses to form a single protostar with significant spiral arms
- The cloud collapses and fragments forming multiple protostars with multiple spiral arms. This scenario is shown in the figure to the left.
Even with this simple model, Boss & Keiser confirm that both magnetic field direction and strength are important in determining the outcome of a molecular cloud. This had already been established with “pseudo-MHD codes”, which are faster than true MHD codes, but the results of these “pseudo-MHD codes” need to be verified with more detailed calculations such as those presented in this paper. In the future, researchers can use Enzo 2.0 to study more complicated star formation structures such as oblate and prolate clouds which better resemble observed molecular clouds.