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arXiv 1007.1078astro-ph.GA
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质量损失率和星团的质量演化

Mass loss rates and the mass evolution of star clusters

Henny J. G. L. M. Lamers, Holger Baumgardt, Mark Gieles

摘要:

基于恒星演化和星团动力学的基本原理以及星团模型的N体模拟网格,我们描述了恒星演化和演化星团动力学质量损失之间的相互作用。这些星系团模型具有不同的初始质量、不同的轨道(包括椭圆轨道)和不同的初始密度分布。我们使用两套集群模型:最初的罗奇叶填充和罗奇叶填充不足。我们确定了四种不同的质量损失效应:(1)由恒星演化引起的质量损失,(2)由恒星演化引起的质量损失和(3)在核心坍缩之前和(4)之后由弛豫驱动的质量损失。演化导致的恒星损失和弛豫驱动的质量损失都需要时间来积累。这是描述的延迟函数的几个交叉时间的罗氏瓣填充集群和几个半质量松弛时间的罗氏瓣欠填充集群。弛豫驱动的质量损失可以用质量dM/dt =-M^{1-gamma}/t0的简单幂律依赖关系来描述,其中t0依赖于星团的轨道和环境。对于King参数W 0 =5的聚类,Gamma为0.65,对于W 0 =7的更集中的聚类,Gamma为0.80。对于最初的罗氏瓣欠填充集群的溶解是由相同的伽玛=0.80。常数t0的值由依赖于星系团轨道的简单公式描述。的质量损失率增加了约一个因素,在核心崩溃和质量依赖性的松弛驱动的质量损失的变化,γ =0.70核心崩溃后。我们还提出了一个简单的配方,用于预测具有各种金属丰度和不同环境的单个星团的质量演化,在大多数情况下,准确率为百分之几。这可以用来预测团簇系统的质量演化。

英文摘要:

We describe the interplay between stellar evolution and dynamical mass loss of evolving star clusters, based on the principles of stellar evolution and cluster dynamics and on a grid of N-body simulations of cluster models. The cluster models have different initial masses, different orbits, including elliptical ones, and different initial density profiles. We use two sets of cluster models: initially Roche-lobe filling and Roche-lobe underfilling. We identify four distinct mass loss effects: (1) mass loss by stellar evolution, (2) loss of stars induced by stellar evolution and (3) relaxation-driven mass loss before and (4) after core collapse. Both the evolution-induced loss of stars and the relaxation-driven mass loss need time to build up. This is described by a delay-function of a few crossing times for Roche-lobe filling clusters and a few half mass relaxation times for Roche-lobe underfilling clusters. The relaxation-driven mass loss can be described by a simple power law dependence of the mass dM/dt =-M^{1-gamma}/t0, (with M in Msun) where t0 depends on the orbit and environment of the cluster. Gamma is 0.65 for clusters with a King-parameter W0=5 and 0.80 for more concentrated clusters with W0=7. For initially Roche-lobe underfilling clusters the dissolution is described by the same gamma=0.80. The values of the constant t0 are described by simple formulae that depend on the orbit of the cluster. The mass loss rate increases by about a factor two at core collapse and the mass dependence of the relaxation-driven mass loss changes to gamma=0.70 after core collapse. We also present a simple recipe for predicting the mass evolution of individual star clusters with various metallicities and in different environments, with an accuracy of a few percent in most cases. This can be used to predict the mass evolution of cluster systems.

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