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HYDRODYNAMIC SIMULATIONS OF H ENTRAINMENT AT THE TOP OF He-SHELL FLASH CONVECTION

机译:He壳对流顶部H夹杂的水动力模拟

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We present the first three-dimensional, fully compressible gas-dynamics simulations in 4π geometry of He-shell flash convection with proton-rich fuel entrainment at the upper boundary. This work is motivated by the insufficiently understood observed consequences of the H-ingestion flash in post-asymptotic giant branch (post-AGB) stars (Sakurai's object) and metal-poor AGB stars. Our investigation is focused on the entrainment process at the top convection boundary and on the subsequent advection of H-rich material into deeper layers, and we therefore ignore the burning of the proton-rich fuel in this study. We find that for our deep convection zone, coherent convective motions of near global scale appear to dominate the flow. At the top boundary convective shear flows are stable against Kelvin-Helmholtz instabilities. However, such shear instabilities are induced by the boundary-layer separation in large-scale, opposing flows. This links the global nature of thick shell convection with the entrainment process. We establish the quantitative dependence of the entrainment rate on grid resolution. With our numerical technique, simulations with 10243 cells or more are required to reach a numerical fidelity appropriate for this problem. However, only the result from the 15363 simulation provides a clear indication that we approach convergence with regard to the entrainment rate. Our results demonstrate that our method, which is described in detail, can provide quantitative results related to entrainment and convective boundary mixing in deep stellar interior environments with very stiff convective boundaries. For the representative case we study in detail, we find an entrainment rate of 4.38 ± 1.48 × 10–13 M ☉ s–1.
机译:我们在He-shell闪蒸对流的4π几何中提出了第一个三维,完全可压缩的气体动力学模拟,在上边界处带有富质子的燃料夹带。这项工作是由于对渐近后的巨型分支(后AGB)恒星(樱井的物体)和贫金属的AGB恒星中的H吸入闪光的后果认识不足而引起的。我们的研究集中在顶部对流边界的夹带过程以及随后富氢物质向更深层的对流,因此我们在本研究中忽略了富质子燃料的燃烧。我们发现,对于我们的深对流区来说,接近整体尺度的相干对流运动似乎主导了流动。在顶部边界处,对流剪切流对开尔文-亥姆霍兹不稳定性是稳定的。但是,这种剪切不稳定性是由边界层分离在大规模,相反的流动中引起的。这将厚壳对流的整体性质与夹带过程联系在一起。我们建立了夹带率对网格分辨率的定量依赖性。使用我们的数值技术,需要使用10243个或更多单元进行仿真,以达到适合此问题的数值保真度。但是,只有15363仿真的结果清楚地表明我们在夹带率方面趋于收敛。我们的结果表明,对我们的方法进行了详细描述,可以在深刚性的对流边界较深的恒星内部环境中提供与夹带和对流边界混合有关的定量结果。对于代表性案例,我们进行了详细研究,发现夹带率为4.38±1.48×10–13 M s s-1。

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