Abstract

Abstract We perform numerical simulations of hydrodynamic (HD) and magnetohydrodynamic (MHD) turbulence driven by compressive driving, to study the generation of solenoidal velocity components and the small-scale magnetic field. We mainly focus on the effects of mean magnetic field (B 0) and the sonic Mach number (M s ). The dependence of solenoidal ratio (i.e., ratio of solenoidal to kinetic energies) and magnetic energy density on M s in compressively driven turbulence is already established, but that on B 0 is not yet. We also consider two different driving schemes in terms of the correlation timescale of forcing vectors: a finite-correlated driving and a delta-correlated driving. Our findings are as follows. First, when we fix the value of B 0, the solenoidal ratio after saturation increases as increases. A similar trend is observed for generation of magnetic field when B 0 is small. Second, when we fix the value of , HD and MHD simulations result in similar solenoidal ratios when B 0 is not strong (say, M A ≳ 5, where M A is Alfvén Mach number). However, the ratio increases when M A ≲ 5. Roughly speaking, the magnetic energy density after saturation is a linearly increasing function of B 0 irrespective of M s . Third, generation of the solenoidal velocity component is not sensitive to numerical resolution, but that of magnetic energy density is mildly sensitive. Finally, when initial conditions are same, the finite-correlated driving always produces more solenoidal velocity and small-scale magnetic field components than the delta-correlated driving. We additionally analyze the vorticity equation to understand why higher and B 0 yield a larger quantity of the solenoidal velocity component.

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