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CN MORPHOLOGY STUDIES OF COMET 103P/HARTLEY 2

机译:CN COMET 103P / HARTLEY 2的形态学

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We report on narrowband CN imaging of Comet 103P/Hartley 2 obtained at Lowell Observatory on 39 nights from 2010 July until 2011 January. We observed two features, one generally to the north and the other generally to the south. The CN morphology varied during the apparition: no morphology was seen in July; in August and September, the northern feature dominated and appeared as a mostly face-on spiral; in October, November, and December, the northern and southern features were roughly equal in brightness and looked like more side-on corkscrews; in January, the southern feature was dominant but the morphology was indistinct due to very low signal. The morphology changed smoothly during each night and similar morphology was seen from night to night. However, the morphology did not exactly repeat each rotation cycle, suggesting that there is a small non-principal axis rotation. Based on the repetition of the morphology, we find evidence that the fundamental rotation period was increasing: 16.7?hr from August 13 to 17, 17.2?hr from September 10 to 13, 18.2?hr from October 12 to 19, and 18.7?hr from October 31 to November 7. We conducted Monte Carlo jet modeling to constrain the pole orientation and locations of the active regions based on the observed morphology. Our preliminary, self-consistent pole solution has an obliquity of 10° relative to the comet's orbital plane (i.e., it is centered near R.A. = 257° and decl. = +67° with an uncertainty around this position of about 15°) and has two mid-latitude sources, one in each hemisphere.
机译:我们报道了从2010年7月至2011年1月的39个晚上在洛厄尔天文台获得的彗星103P /哈特利2号彗星的窄带CN成像。我们观察到两个特征,一个特征通常位于北部,另一个特征通常位于南部。幻影过程中CN形态发生变化:7月未见形态。在八月和九月,北部地区占主导地位,并呈现出一个几乎面朝上的螺旋状。在10月,11月和12月,北部和南部的特征在亮度上大致相等,看起来像是更多的侧面开瓶器。一月,南部特征占主导地位,但由于信号极低,其形态不明显。形态在每个晚上都平稳变化,并且从夜晚到夜晚都观察到相似的形态。但是,形态没有完全重复每个旋转周期,这表明存在一个小的非主轴旋转。根据形态的重复,我们发现证据表明基本旋转周期正在增加:从8月13日至17日为16.7小时,从9月10日至13日为17.2小时,从10月12日至19日为18.2小时,并且是18.7小时。从10月31日至11月7日。我们进行了蒙特卡洛射流建模,以根据观察到的形态来约束极区的方向和活动区域的位置。我们初步的,自洽的极点解相对于彗星轨道平面的倾角为10°(即,其中心位于RA = 257°和decl。= + 67°附近,该位置周围的不确定性约为15°),并且有两个中纬度源,每个半球一个。

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