论文标题
对流驱动的大恒星信封中的三维湍流:I。扩散辐射传输的一维实施
Convectively Driven Three Dimensional Turbulence in Massive Star Envelopes: I. A 1D Implementation of Diffusive Radiative Transport
论文作者
论文摘要
巨大的($ m> 30 \,$ m $ _ {\ odot} $)星星表现出在Eddington-limit的电子散射附近,导致与铁的不透明度增加在$ t \ t \ t \ t \ th \ t \ th \ t \ th $ t \ of180,000 \,$ k相关的不透明度上,以触发其外部信封中的超音速对流。江安的三维辐射流体动力学模拟和与雅典娜++计算工具的合作者在这些对流区域中发现了数量级密度和辐射通量波动的顺序,即使在光学深度$ \ gg100 $也是如此。我们在这里表明,在对流的时间表中,辐射可以从包裹中扩散出来,从而激发了我们使用“伪”马赫数以表征波动振幅及其相关性的表征。在第一篇论文中,我们得出了这些波动对携带给定辐射光度所需的辐射压力梯度的影响。这种实现会导致1D和3D辐射压力梯度之间的显着改善,并建立了我们对这些本质上3D信封的最终1D实施道路的信心。但是,简单地降低辐射压力梯度不足以实现新的1D模型。相反,我们还必须说明湍流对流的其他两个方面的影响:巨大的压力和运输可观的亮度部分的能力,这将在即将到来的作品中解决。在其他情况下,恒星光度接近爱丁顿光度的其他情况也出现了这种湍流对流。因此,我们的努力应适用于其他天体物理情况,在近乎爱丁顿有限的辐射压力主导的等离子体中出现不透明峰。
Massive ($M >30\,$M$_{\odot}$) stars exhibit luminosities that are near the Eddington-limit for electron scattering causing the increase in opacity associated with iron at $T\approx180,000\,$K to trigger supersonic convection in their outer envelopes. Three dimensional radiative hydrodynamics simulations by Jiang and collaborators with the Athena++ computational tool have found order of magnitude density and radiative flux fluctuations in these convective regions, even at optical depths $\gg100$. We show here that radiation can diffuse out of a parcel during the timescale of convection in these optically thick parts of the star, motivating our use of a "pseudo" Mach number to characterize both the fluctuation amplitudes and their correlations. In this first paper, we derive the impact of these fluctuations on the radiative pressure gradient needed to carry a given radiative luminosity. This implementation leads to a remarkable improvement between 1D and 3D radiative pressure gradients, and builds confidence in our path to an eventual 1D implementation of these intrinsically 3D envelopes. However, simply reducing the radiation pressure gradient is not enough to implement a new 1D model. Rather, we must also account for the impact of two other aspects of turbulent convection: the substantial pressure, and the ability to transport an appreciable fraction of the luminosity, which will be addressed in upcoming works. This turbulent convection also arises in other instances where the stellar luminosity approaches the Eddington luminosity. Hence, our effort should apply to other astrophysical situations where an opacity peak arises in a near Eddington limited, radiation pressure dominated plasma.