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首页> 外文期刊>The Astrophysical journal >Newtonian Hydrodynamics of the Coalescence of Black Holes with Neutron Stars. I. Tidally Locked Binaries with a Stiff Equation of State
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Newtonian Hydrodynamics of the Coalescence of Black Holes with Neutron Stars. I. Tidally Locked Binaries with a Stiff Equation of State

机译:黑洞与中子星合并的牛顿流体动力学。 I.具有刚性状态方程的潮汐锁定二进制

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We present a detailed Newtonian study of the last stages of binary evolution of a black hole and a neutron star, when the components are separated by a few stellar radii. Our simulations are carried out using a three-dimensional smooth particle hydrodynamics (SPH) code. We calculate the gravitational radiation waveforms as well as the gravitational radiation luminosity in the quadrupole approximation. The neutron star is modeled with a stiff polytropic equation of state, P = KρΓ, with the adiabatic index Γ = 3. We have performed runs with two different resolutions, using 16,944 and 8121 particles initially. Our equilibrium initial conditions correspond to tidally locked binaries with different initial values of the mass ratio q = M/MBH (where M is the mass of the neutron star and MBH is that of the black hole). The dynamical evolution of the system was simulated using an ideal gas equation of state for a time equivalent to several initial orbital periods. We find that for high mass ratios (q = 1 and q = 0.8, but not for q = 0.31) there is a critical separation at which the binary becomes unstable due to hydrodynamical effects and decays on a dynamical timescale. The neutron star is not completely tidally disrupted, and its core continues to orbit the black hole. For a mass ratio of unity, an accretion torus forms around the black hole and survives for several dynamical times, but no comparable accretion structure is present for lower mass ratios. For q = 0.31 we have performed two separate runs, one with gravitational radiation reaction included in our calculations, and one with no gravitational radiation reaction—in both cases we find intermittent mass transfer through Roche lobe overflow. For the stiff polytrope considered here, the binary system always survives the initial mass transfer—the encounter results in a decreased mass ratio and increased separation. In all cases, the binary axis is free of baryons.
机译:当组件被几个恒星半径分开​​时,我们将对牛顿和中子星二元演化的最后阶段进行详细的牛顿研究。我们的仿真是使用三维光滑粒子流体动力学(SPH)代码进行的。我们以四极近似计算引力辐射波形以及引力辐射亮度。中子星是用一个刚性的多态状态方程P =KρΓ和绝热指数Γ= 3来建模的。我们以两种不同的分辨率进行了运行,最初使用了16,944和8121个粒子。我们的平衡初始条件对应于质量比q = M / MBH(其中M是中子星质量,MBH是黑洞质量)的初始值不同的潮汐锁定双星。使用理想的气体状态方程在相当于几个初始轨道周期的时间内模拟了系统的动态演化。我们发现,对于高质量比(q = 1和q = 0.8,而不是q = 0.31),存在临界分离,在该临界分离下,二元化合物由于流体动力学效应而变得不稳定,并在动态时标上衰减。中子星没有被潮汐波彻底破坏,它的核心继续绕黑洞运行。对于统一的质量比,吸积环在黑洞周围形成并存活数次,但是对于较低的质量比,不存在可比的吸积结构。对于q = 0.31,我们执行了两个单独的运行,一个运行包含在我们的计算中,其中有重力辐射反应,另一个没有重力辐射反应,在这两种情况下,我们都发现了通过罗氏波瓣溢流的间歇传质。对于此处考虑的刚性多形体而言,二元系统始终在初始质量传递过程中幸免于难,因为相遇会导致质量比降低和分离度提高。在所有情况下,二进制轴都没有重子。

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