论文标题
磁化振荡的双向对流
Magnetized oscillatory double-diffusive convection
论文作者
论文摘要
我们研究了在存在均匀的垂直背景磁场的情况下振荡性双扩散对流(ODDC)的特性。 ODDC发生在恒星区域,根据Schwarzschild标准不稳定,并根据Ledoux标准(有时称为半感染区域)进行稳定,通常预测它们仅位于中等质量主序列星的核心之外。先前对ODDC的流体动力学研究表明,基本的不稳定性饱和成类似波浪的对流状态,但是二次不稳定性有时可以将其转化为分层对流的状态,然后层迅速合并并成长直到整个区域完全对流。我们发现,磁化ODDC总体上具有非常相似的属性,并且存在一些重要的定量差异。线性稳定性分析表明,增长最快的模式不受场地的影响,但其他模式是。从数值上讲,磁场被认为会影响基本不稳定性的饱和度,总体上减少了温度和成分的湍流。反过来,这会影响层的形成,通常会延迟其形成,并偶尔将其完全抑制为足够强的场。但是,将需要进一步的工作来确定在哪个实际上抑制恒星中层形成的场强度。简要讨论了潜在的观察意义。
We study the properties of oscillatory double-diffusive convection (ODDC) in the presence of a uniform vertical background magnetic field. ODDC takes place in stellar regions that are unstable according to the Schwarzschild criterion and stable according to the Ledoux criterion (sometimes called semiconvective regions), which are often predicted to reside just outside the core of intermediate-mass main sequence stars. Previous hydrodynamic studies of ODDC have shown that the basic instability saturates into a state of weak wave-like convection, but that a secondary instability can sometimes transform it into a state of layered convection, where layers then rapidly merge and grow until the entire region is fully convective. We find that magnetized ODDC has very similar properties overall, with some important quantitative differences. A linear stability analysis reveals that the fastest-growing modes are unaffected by the field, but that other modes are. Numerically, the magnetic field is seen to influence the saturation of the basic instability, overall reducing the turbulent fluxes of temperature and composition. This in turn affects layer formation, usually delaying it, and occasionally suppressing it entirely for sufficiently strong fields. Further work will be needed, however, to determine the field strength above which layer formation is actually suppressed in stars. Potential observational implications are briefly discussed.