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首页> 外文期刊>The Astrophysical journal >EQUILIBRIUM CONFIGURATIONS OF SYNCHRONOUS BINARIES: NUMERICAL SOLUTIONS AND APPLICATION TO KUIPER BELT BINARY 2001 QG298
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EQUILIBRIUM CONFIGURATIONS OF SYNCHRONOUS BINARIES: NUMERICAL SOLUTIONS AND APPLICATION TO KUIPER BELT BINARY 2001 QG298

机译:同步双二进制的均衡配置:数值解法及其在Kuiper Belt Binary 2001 QG298中的应用

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We present numerical computations of the equilibrium configurations of tidally locked homogeneous binaries rotating in circular orbits. Unlike the classical Roche approximations, we self-consistently account for the tidal and rotational deformations of both components, and relax the assumptions of ellipsoidal configurations and Keplerian rotation. We find numerical solutions for mass ratios q between 10–3 and 1, starting at a small angular velocity for which tidal and rotational deformations are small, and following a sequence of increasing angular velocities. Each series terminates at an appropriate "Roche limit," above which no equilibrium solution can be found. Even though the Roche limit is crossed before the "Roche lobe" is filled, any further increase in the angular velocity will result in mass-loss. For close, comparable-mass binaries, we find that local deviations from ellipsoidal forms may be as large as 10%-20%, and departures from Keplerian rotation are significant. We compute the light curves that arise from our equilibrium configurations, assuming their distance is 1?AU (e.g., in the Kuiper Belt). We consider both backscatter (proportional to the projected area) and diffuse (Lambert) reflections. Backscatter reflection always yields two minima of equal depths. Diffuse reflection, which is sensitive to the surface curvature, generally gives rise to unequal minima. We find detectable intensity differences of up to 10% between our light curves and those arising from the Roche approximations. Finally, we apply our models to Kuiper Belt binary 2001 QG298, and find a nearly edge-on binary with a mass ratio q = 0.93+0.07 –0.03, angular velocity ω2/Gρ = 0.333 ± 0.001 (statistical errors only), and pure diffuse reflection. For the observed period of 2001 QG298, these parameters imply a bulk density ρ = 0.72 ± 0.04 g cm–3.
机译:我们提出了在圆形轨道上旋转的潮汐锁定均质二元平衡构型的数值计算。与经典的罗氏近似不同,我们始终如一地考虑两个分量的潮汐和旋转变形,并放宽了椭圆形构型和开普勒旋转的假设。我们发现质量比q在10–3和1之间的数值解开始于一个小角速度,对于该小角速度而言,潮汐和旋转变形较小,并且随着角速度的增加而增加。每个系列都在适当的“罗氏极限”处终止,在该极限以上找不到平衡解。即使在填充“罗氏波瓣”之前已超过罗氏极限,但角速度的任何进一步增加都将导致质量损失。对于接近的,可比较质量的二进制文件,我们发现与椭球形式的局部偏差可能高达10%-20%,并且与开普勒旋转的偏差很大。假设它们的距离为1?AU(例如在柯伊伯带中),我们将计算由平衡配置产生的光曲线。我们考虑了反向散射(与投影区域成比例)和漫反射(兰伯特)反射。反向散射反射始终会产生两个深度相等的最小值。对表面曲率敏感的漫反射通常会导致不相等的最小值。我们发现,我们的光曲线与罗氏近似值之间可检测到的强度差异高达10%。最后,我们将模型应用于Kuiper Belt二进制2001 QG298,找到质量比为q = 0.93 + 0.07 –0.03,角速度ω2/Gρ= 0.333±0.001(仅统计误差)且纯净的近边缘二进制漫反射。对于2001年QG298的观测时期,这些参数意味着堆积密度ρ= 0.72±0.04 g cm–3。

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