论文标题
在可压缩等温湍流的直接数值模拟中磁性螺旋性的反向转移:缩放定律
Inverse transfer of magnetic helicity in direct numerical simulations of compressible isothermal turbulence: scaling laws
论文作者
论文摘要
通过在等温理想磁性水力学(MHD)框架中的大规模机械驱动的湍流(MHD)框架中的大规模机械驱动的湍流的直接数值模拟研究了磁性螺旋度的反转移。机械强迫要么是纯螺旋桨或纯压缩的,而且湍流的稳态被认为是均方根(RMS)马赫数为0.1 $ \ sillsim $ m $ \ m $ \ lysesim $11。一种连续的小型电动电动强迫注入磁性直升机波动,从而导致较大的磁性结构的堆积。观察到光谱缩放指数,对于低马赫数,这与不可压缩情况下的先前研究一致。较高的可压缩性会导致磁性螺旋性缩放指数。与不可压缩的情况相比,与可压缩的湍流相比,与不可压缩的情况相比,与压缩驱动的湍流相比,即使在高马赫数处的偏差也相对较小,在压缩驱动的湍流中,在相对温和的RMS MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH MACH-GTRSIM $ 3中,可压缩效应在磁性旋转时可以在压缩的情况下起重要作用。但是,在不可压缩的情况下观察到的理论结果可以通过使用AlfVén速度代替磁场,将变量的适当变化转移到超音速湍流中。
The inverse transfer of magnetic helicity is investigated through direct numerical simulations of large-scale-mechanically-driven turbulent flows in the isothermal ideal magnetohydrodynamics (MHD) framework. The mechanical forcing is either purely solenoidal or purely compressive and the turbulent steady-states considered exhibit root mean square (RMS) Mach numbers 0.1 $\lesssim$ M $\lesssim$ 11. A continuous small-scale electromotive forcing injects magnetic helical fluctuations, which lead to the build-up of ever larger magnetic structures. Spectral scaling exponents are observed which, for low Mach numbers, are consistent with previous research done in the incompressible case. Higher compressibility leads to flatter magnetic helicity scaling exponents. The deviations from the incompressible case are comparatively small for solenoidally-driven turbulence, even at high Mach numbers, as compared to those for compressively-driven turbulence, where strong deviations are already visible at relatively mild RMS Mach numbers M $\gtrsim$ 3. Compressible effects can thus play an important role in the inverse transfer of magnetic helicity, especially when the turbulence drivers are rather compressive. Theoretical results observed in the incompressible case can, however, be transferred to supersonic turbulence by an appropriate change of variables, using the Alfvén velocity in place of the magnetic field.