Scaling laws of passive-scalar diffusion in the interstellar medium

被引:43
|
作者
Colbrook, Matthew J. [1 ]
Ma, Xiangcheng [2 ]
Hopkins, Philip F. [2 ]
Squire, Jonathan [2 ,3 ]
机构
[1] Univ Cambridge, Dept Appl Math & Theoret Phys, Cambridge CB3 0WA, England
[2] CALTECH, TAPIR, Mailcode 350-17, Pasadena, CA 91125 USA
[3] Walter Burke Inst Theoret Phys, Pasadena, CA 91125 USA
关键词
diffusion; methods: analytical; methods: numerical; stars: formation; ISM: evolution; galaxies: formation; ANOMALOUS DIFFUSION; TURBULENCE; DRIVEN; STATISTICS; SIMULATIONS; ENRICHMENT; TRANSPORT; ACCURATE; ORIGIN;
D O I
10.1093/mnras/stx261
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Passive-scalar mixing (metals, molecules, etc.) in the turbulent interstellar medium (ISM) is critical for abundance patterns of stars and clusters, galaxy and star formation, and cooling from the circumgalactic medium. However, the fundamental scaling laws remain poorly understood in the highly supersonic, magnetized, shearing regime relevant for the ISM. We therefore study the full scaling laws governing passive-scalar transport in idealized simulations of supersonic turbulence. Using simple phenomenological arguments for the variation of diffusivity with scale based on Richardson diffusion, we propose a simple fractional diffusion equation to describe the turbulent advection of an initial passive scalar distribution. These predictions agree well with the measurements from simulations, and vary with turbulent Mach number in the expected manner, remaining valid even in the presence of a large-scale shear flow (e.g. rotation in a galactic disc). The evolution of the scalar distribution is not the same as obtained using simple, constant 'effective diffusivity' as in Smagorinsky models, because the scale dependence of turbulent transport means an initially Gaussian distribution quickly develops highly non-Gaussian tails. We also emphasize that these are mean scalings that apply only to ensemble behaviours (assuming many different, random scalar injection sites): individual Lagrangian 'patches' remain coherent (poorly mixed) and simply advect for a large number of turbulent flow-crossing times.
引用
收藏
页码:2421 / 2429
页数:9
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