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EQUATORIAL WIND COMPRESSION EFFECTS ACROSS THE H-R DIAGRAM

机译:沿H-R图的赤道风压效应

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We investigate the degree to which moderate stellar rotation rates can influence the two-dimensional density structure in the winds of four classes of stars: Wolf-Rayet, B[e], asymptotic giant branch (AGB), and novae. These classes are distributed across the H-R diagram and have a wide range of escape speeds and wind acceleration. Furthermore, all have members which possess asymmetric circumstellar nebulae. It has been suggested that these asymmetries could result from stellar winds which have moderate equatorial density enhancements. Large enhancements may arise as the result of stellar rotation as demonstrated by the wind-compressed disk (WCD) model of Bjorkman & Cassinelli. Instead of a dense disk, here we consider a milder distortion called a wind-compressed zone (WCZ), A WCZ is said to occur if a star rotates more slowly than the disk formation threshold and if the density at the equator is more than about 3 times that at the pole. We assume that the stellar winds obey a standard β-velocity law and consider the effects of varying two of the velocity law parameters: the terminal speed, v_∞, and the exponent, β. For a given rotation rate, the wind compression is enhanced as either v_∞ is decreased or β is increased, because both correspond to a smaller acceleration of the wind. A general result from our model simulations is that the asymptotic density and flow structure are predominantly governed by the ratio ω/ω_D, where ω is the stellar rotation rate normalized to the critical speed and ω_D is the threshold value needed for disk formation. For the Wolf-Rayet and B[e] models which have moderate wind terminal speeds and shallow velocity laws (β= 3), a WCZ can form even at rotation rates of order 10% and 20% critical, respectively. For the AGB model with a low terminal speed and a β = 3 velocity law, a WCZ can form at 15% critical. Finally, we consider novae, which have time-variable wind properties. In particular, the location of the sonic point is time dependent, so we compute models with a range of sonic point radii. In favorable cases, a WCZ can form for white dwarf rotation rates of less than 20% critical; however, further work will be required to properly treat the extended subsonic region of nova winds.
机译:我们研究了适度的恒星自转速率可影响四类恒星的风中的二维密度结构的程度:沃尔夫-雷耶特,B [e],渐近巨星分支(AGB)和新星。这些类别分布在H-R图表上,具有广泛的逃生速度和风加速度。此外,所有成员都具有不对称的星状星云。已经提出这些不对称性可能是由恒星风引起的,该恒星风具有中等赤道密度的增强作用。如Bjorkman&Cassinelli的风压盘(WCD)模型所显示的,恒星旋转的结果可能会产生很大的增强。代替密集的磁盘,这里考虑的是称为风压缩区(WCZ)的轻微失真,如果恒星的旋转速度慢于磁盘形成阈值,并且赤道的密度大于约200°C,则称为WCZ。在极点的3倍。我们假设恒星风服从标准的β速度定律,并考虑了两个速度定律参数的变化的影响:终极速度v_∞和指数β。对于给定的旋转速度,由于v_∞减小或β增加,因此风的压缩增强,因为两者都对应于较小的风加速度。我们的模型仿真的总体结果是,渐进密度和流动结构主要由比率ω/ω_D决定,其中ω是归一化为临界速度的恒星旋转速率,而ω_D是形成圆盘所需的阈值。对于具有适中的风终端速度和较浅的速度定律(β= 3)的Wolf-Rayet和B [e]模型,甚至在临界转速分别为10%和20%的情况下也可以形成WCZ。对于具有低终端速度和β= 3速度定律的AGB模型,WCZ的临界形成率为15%。最后,我们考虑新星,它具有随时间变化的风属性。特别是,声波点的位置与时间有关,因此我们可以计算具有一定范围的声波点半径的模型。在有利的情况下,WCZ可以形成小于20%临界值的白矮星自转;然而,将需要进一步的工作来适当地处理新星风的扩展亚音速区域。

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