4.7 Article

Turbulent mixing and nuclear burning in stellar interiors

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 481, Issue 3, Pages 2918-2932

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/sty2392

Keywords

hydrodynamics; turbulence; stars: evolution; stars: interiors

Funding

  1. Los Alamos National Laboratory
  2. University of Arizona
  3. Australian Research Council [FT160100046]
  4. Australian Government through NCI via the National Computational Merit Allocation Scheme [ew6]
  5. Theoretical Astrophysics Program (TAP)
  6. Steward Observatory
  7. Australian Research Council [FT160100046] Funding Source: Australian Research Council

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The turbulent burning of nuclei is a common phenomenon in the evolution of stars. Here we examine a challenging case: the merging of the neon and oxygen burning shells in a 23 M-circle dot star. A previously unknown quasi-steady state is established by the interplay between mixing, turbulent transport, and nuclear burning. The resulting stellar structure has two burning shells within a single convection zone. We find that the new neon burning layer covers an extended region of the convection zone, with the burning peak occurring substantially below where the average convective turnover timescale becomes equal to the burning timescale. These characteristics differ from those predicted by 1D stellar evolution models of similar ingestion events. We develop the mean-field turbulence equations that govern compositional evolution, and use them to interpret our data set. An important byproduct is a means to quantify sub-grid-scale effects intrinsic to the numerical hydrodynamic scheme. For implicit large eddy simulations, the analysis method is particularly powerful because it can reveal where and how simulated flows are modified by resolution, and provide straightforward physical interpretations of the effects of dissipation or induced transport. Focusing on the mean-field composition variance equations for our analysis, we recover a Kolmogorov rate of turbulent dissipation without it being imposed, in agreement with previous results which used the turbulent kinetic energy equation.

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