首页> 外文期刊>The Astrophysical journal >STATISTICS OF CORE LIFETIMES IN NUMERICAL SIMULATIONS OF TURBULENT, MAGNETICALLY SUPERCRITICAL MOLECULAR CLOUDS
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STATISTICS OF CORE LIFETIMES IN NUMERICAL SIMULATIONS OF TURBULENT, MAGNETICALLY SUPERCRITICAL MOLECULAR CLOUDS

机译:湍流,磁超临界分子的数值模拟中的核心寿命统计

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摘要

We present measurements of the mean dense core lifetimes in numerical simulations of magnetically supercritical, turbulent, isothermal molecular clouds, in order to compare with observational determinations. "Prestellar" lifetimes are consistent with observationally reported values, ranging from a few to several free-fall times. We also present estimates of the fraction of cores in the "prestellar," "stellar," and "failed" (those cores that redisperse back into the environment) stages as a function of the threshold density used to define them, n_(thr). The number ratios are measured indirectly in the simulations, due to resolution limitations. Our approach contains one free parameter, the lifetime of a protostellar object, T_(yso) (Class 0 + Class Ⅰ stages), that is outside the realm of the simulations. Assuming a value of T_(yso) = 0.46 Myr, we obtain number ratios of starless to stellar cores ranging from 4-5 at n_(thr) = 1.5 × 10~4 cm~(-3) to ~1 at n_(thr) = 1.2 × 10~5 cm~(-3), again in good agreement with observational determinations. We also find that the mass in the failed cores is comparable to that in stellar cores at n_(thr) = 1.5 × 10~4 cm~(-3), but becomes negligible at n_(thr) = 1.2 × 10~5 cm~(-3), in agreement with recent observational suggestions that at the latter densities the cores are in general gravitationally dominated. We conclude by noting that the timescale for core contraction and collapse is virtually the same in the subcritical, ambipolar diffusion-mediated model of star formation, in the model of star formation in turbulent supercritical clouds, and in a model intermediate between the previous two for currently accepted values of the clouds' magnetic criticality.
机译:我们在磁超临界,湍流,等温分子云的数值模拟中提供了平均密集堆芯寿命的测量结果,以便与观测结果进行比较。 “星际”的寿命与观察到的值一致,从几到几次自由落体时间。我们还根据“阈值密度” n_(thr)的函数,给出了“星状”,“星状”和“失效”(重新散布回环境的那些岩心)阶段中岩心分数的估计值。 。由于分辨率的限制,数比是在模拟中间接测量的。我们的方法包含一个自由参数,即恒星对象T_(yso)的寿命(0级+Ⅰ级),这超出了模拟范围。假设T_(yso)= 0.46 Myr的值,我们得到的无星核与恒星核的数量比在n_(thr)= 1.5×10〜4 cm〜(-3)的4-5到n_(thr)的〜1 )= 1.2×10〜5 cm〜(-3),再次与观测值吻合。我们还发现,在n_(thr)= 1.5×10〜4 cm〜(-3)时,失效核的质量与恒星核的质量相当,但在n_(thr)= 1.2×10〜5 cm的质量可忽略不计〜(-3)与最近的观测建议一致,即在后一种密度下,岩心通常在重力作用下占主导地位。我们的结论是,在亚临界,双极扩散介导的恒星形成模型,湍流超临界云中的恒星形成模型以及前两者之间的中间模型中,核心收缩和塌陷的时间尺度实际上是相同的。目前公认的云磁临界值。

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