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首页> 外文期刊>Icarus: International Journal of Solar System Studies >Binary asteroid population. 2. Anisotropic distribution of orbit poles of small, inner main-belt binaries
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Binary asteroid population. 2. Anisotropic distribution of orbit poles of small, inner main-belt binaries

机译:二元小行星种群。 2.小​​型内部主带双星的轨道极的各向异性分布

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摘要

Our photometric observations of 18 main-belt binary systems in more than one apparition revealed a strikingly high number of 15 having positively re-observed mutual events in the return apparitions. Our simulations of the survey showed that it cannot be due to an observational selection effect and that the data strongly suggest that poles of mutual orbits between components of binary asteroids in the primary size range 3-8. km are not distributed randomly: The null hypothesis of an isotropic distribution of the orbit poles is rejected at a confidence level greater than 99.99%. Binary orbit poles concentrate at high ecliptic latitudes, within 30° of the poles of the ecliptic. We propose that the binary orbit poles oriented preferentially up/down-right are due to either of the two processes: (i) the YORP tilt of spin axes of their parent bodies toward the asymptotic states near obliquities 0° and 180° (pre-formation mechanism) or (ii) the YORP tilt of spin axes of the primary components of already formed binary systems toward the asymptotic states near obliquities 0° and 180° (post-formation mechanism). The alternative process of elimination of binaries with poles closer to the ecliptic by dynamical instability, such as the Kozai effect due to gravitational perturbations from the Sun, does not explain the observed orbit pole concentration. This is because for close binary asteroid systems, the gravitational effects of primary's irregular shape dominate the solar-tide effect.
机译:我们在一个以上的幻影中对18个主皮带二元系统进行了光度学观察,结果发现,在回归幻影中有15个具有积极的重新观察到的相互事件,这一数字惊人地高。我们对调查的模拟表明,这不可能归因于观测选择效应,并且该数据强烈表明,主要大小为3-8的二元小行星组成部分之间的相互轨道极点。 km并非随机分布:轨道极点各向同性分布的零假设在置信度大于99.99%时被拒绝。双轨轨道极点集中在高黄道纬度内,在黄道极的30°以内。我们认为,优先选择向右/向右定向的二元轨道极点是由于以下两个过程之一:(i)其母体自旋轴的YORP倾斜朝向0°和180°倾斜附近的渐近状态(预或(ii)已形成的二元系统主要成分的自旋轴的YORP倾斜朝向0°和180°倾斜附近的渐近状态(后形成机制)。通过动态不稳定性消除极点接近黄道的双星的替代过程,例如由于太阳引力扰动引起的Kozai效应,不能解释观测到的轨道极点浓度。这是因为对于紧密的双星小行星系统,原初的不规则形状的引力作用主导着太阳潮汐作用。

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