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Lobate impact melt flows within the extended ejecta blanket of Pierazzo crater

机译:Lobate撞击熔体流动在皮埃拉泽州火山口的延长喷射物毯子内

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摘要

Impact melt flows are observed within the continuous and discontinuous ejecta blanket of the 9 km lunar crater Pierazzo, from the crater rim to more than 40 km away from the center of the crater. Our mapping, fractal analysis, and thermal modeling suggest that melt can be emplaced ballistically and, upon landing, can become separated from solid ejecta to form the observed flow features. Our analysis is based on the identification of established melt morphology for these in-ejecta flows and supported by fractal analysis and thermal modeling. We computed the fractal dimension for the flow boundaries and found values of D = 1.05–1.17. These are consistent with terrestrial basaltic lava flows (D = 1.06–1.2) and established lunar impact melt flows (D = 1.06–1.18), but inconsistent with lunar dry granular flows (D = 1.31–1.34). Melt flows within discontinuous ejecta deposits are noted within just 1.5% of the mapping area, suggesting that the surface expression of impact melt in the extended ejecta around craters of this size is rare, most likely due to the efficient mixing of melts with solid ejecta and local target rocks. However, if the ejected fragments (both, molten and solid) are large enough, segregation of melt and its consequent flow is possible. As most of the flows mapped in this work occur on crater-facing slopes, the development of defined melt flows within ejecta deposits might be facilitated by high crater-facing topography restricting the flow of ejecta soon after it makes ground contact, limiting the quenching of molten ejecta through turbulent mixing with solid debris. Our study confirms the idea that impact melt can travel far beyond the continuous ejecta blanket, adding to the lunar regolith over an extensive area.
机译:冲击熔融流的9公里月球坑Pierazzo的连续和不连续喷出物内毯观察到,从火山口边缘到超过40公里的火山口的中心。我们的映射,分形分析,和热模型表明,熔体可被布设弹道,并且在着陆,可以成为从固体喷出物分离以形成所观察到的流动特性的部件。我们的分析是基于对这些在-喷出物流建立熔体形态的识别和通过分形分析和热建模支持。我们计算分形维数为流动边界,发现d = 1.05-1.17的值。这些是与地面玄武岩熔岩流一致(d = 1.06-1.2),并建立月球冲击熔体流动(d = 1.06-1.18),但不符合月球干燥颗粒流(d = 1.31-1.34)。熔体连续喷出物沉积物的映射区域的仅1.5%的范围内注意内流动,这表明冲击的表面表达在扩展喷出物的熔体围绕着该尺寸的弹坑是罕见的,很可能是由于熔化的固体喷出物的有效混合和本地目标岩石。但是,如果喷射的片段(包括,熔融金属和固体)是足够大的,熔体和偏析其随之而来的流动是可能的。由于大部分的在该工作流映射发生在朝向火山口的斜坡,限定喷出物沉积物内的熔体流动可能是由高面向火山口地形限制喷出物的它使得地面接触后不久的流动变得容易,限制的淬火发展通过湍流熔融喷出物与固体碎片混合。我们的研究证实的想法,影响熔体可以走很远超出了连续喷出物覆盖,在广阔的区域增加了月壤。

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