论文标题
超音速湍流和密度分布函数的性质
Nature of supersonic turbulence and density distribution function in the multiphase interstellar medium
论文作者
论文摘要
星际介质(ISM)中的超音速流被认为是分子云形成和进化的关键驱动力。在分子云的特性中,湍流的螺线管和压缩模式之间的比率在确定恒星形成效率方面起着重要作用。我们使用暖中性培养基(WNM)的超音速收敛流的数值模拟,以解决热不稳定性以计算分子云形成的早期阶段,并研究多层ISM的湍流结构和密度分布函数(密度PDF)。我们发现螺线管和压缩模式都具有与Kolmogorov频谱相似的功率谱。螺线管(压缩)模式的总湍流功率>约80%(<〜20%)。 When we consider both the cold neutral medium (CNM) and the thermally unstable neutral medium (UNM) up to T <~ 400 K, the density PDF follows the log-normal distribution whose width sigma_s is well explained by the known relation from the isothermal turbulence as sigma_s = ln(1 + b^2 * M^2) (where b is the parameter representing the turbulence mode ratio and M is the turbulent马赫数)。然而,仅CNM组件的密度PDF(T <= 50 K)表现出较窄的sigma_s率〜2。这些结果表明,基于CNM密度PDF的B的观察性估计需要每个CNM内部的内部湍流,但不需要与unf thit wn的unf the wn的cnm cnm团块内的内部湍流。
Supersonic flows in the interstellar medium (ISM) are believed to be a key driver of the molecular cloud formation and evolution. Among molecular clouds' properties, the ratio between the solenoidal and compressive modes of turbulence plays important roles in determining the star formation efficiency. We use numerical simulations of supersonic converging flows of the warm neutral medium (WNM) resolving the thermal instability to calculate the early phase of molecular cloud formation, and investigate the turbulence structure and the density probability distribution function (density PDF) of the multiphase ISM. We find that both the solenoidal and compressive modes have their power spectrum similar to the Kolmogorov spectrum. The solenoidal (compressive) modes account for >~80% (<~20%) of the total turbulence power. When we consider both the cold neutral medium (CNM) and the thermally unstable neutral medium (UNM) up to T <~ 400 K, the density PDF follows the log-normal distribution whose width sigma_s is well explained by the known relation from the isothermal turbulence as sigma_s = ln(1 + b^2 * M^2) (where b is the parameter representing the turbulence mode ratio and M is the turbulent Mach number). The density PDF of the CNM component alone (T <= 50 K), however, exhibits a narrower sigma_s by a factor of ~ 2. These results suggest that observational estimations of b based on the CNM density PDF requires the internal turbulence within each CNM clump but not the inter-clump relative velocity, the latter of which is instead powered by the WNM/UNM turbulence.