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Stardust interstellar dust calibration: Hydrocode modeling of impacts on Al-1100 foil at velocities up to 300kms ~(-1) and validation with experimental data

机译:星尘星际尘埃校准:在300 kms〜(-1)的速度下对Al-1100铝箔撞击的水力代码建模,并通过实验数据进行验证

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We present initial results from hydrocode modeling of impacts on Al-1100 foils, undertaken to aid the interstellar preliminary examination (ISPE) phase for the NASA Stardust mission interstellar dust collector tray. We used Ansys' AUTODYN to model impacts of micrometer-scale, and smaller projectiles onto Stardust foil (100μm thick Al-1100) at velocities up to 300kms -1. It is thought that impacts onto the interstellar dust collector foils may have been made by a combination of interstellar dust particles (ISP), interplanetary dust particles (IDP) on comet, and asteroid derived orbits, β micrometeoroids, nanometer dust in the solar wind, and spacecraft derived secondary ejecta. The characteristic velocity of the potential impactors thus ranges from 1 to a few kms -1 (secondary ejecta), approximately 4-25kms -1 for ISP and IDP, up to hundreds of kms -1 for the nanoscale dust reported by Meyer-Vernet et al. (2009). There are currently no extensive experimental calibrations for the higher velocity conditions, and the main focus of this work was therefore to use hydrocode models to investigate the morphometry of impact craters, as a means to determine an approximate impactor speed, and thus origin. The model was validated against existing experimental data for impact speeds up to approximately 30kms -1 for particles ranging in density from 2.4kgm -3 (glass) to 7.8kgm -3 (iron). Interpolation equations are given to predict the crater depth and diameter for a solid impactor with any diameter between 100nm and 4μm and density between 2.4 and 7.8kg m -3.
机译:我们介绍了对Al-1100铝箔的影响进行水力代码建模的初步结果,旨在帮助NASA星尘号任务星际集尘器托盘进行星际初步检查(ISPE)阶段。我们使用Ansys的AUTODYN建模了微米级的撞击,并将较小的弹丸以高达300kms -1的速度投射到星尘箔(厚度为100μm的Al-1100)上。据认为,对星际集尘器箔片的影响可能是由星际尘埃颗粒(ISP),彗星上的行星际尘埃颗粒(IDP)以及小行星衍生的轨道,β微型流星体,太阳风中的纳米尘埃组合而成的,和宇宙飞船派生的次级弹射器因此,潜在撞击器的特征速度范围从 1到几kms -1(二次喷射),对于ISP和IDP约为4-25kms -1,对于由Meyer- Vernet等。 (2009)。目前尚无针对较高速度条件的广泛实验校准,因此,这项工作的主要重点是使用液压编码模型研究撞击坑的形态,以此来确定近似撞击器速度,从而确定撞击源。针对密度范围从2.4kgm -3(玻璃)到7.8kgm -3(铁)的颗粒,该模型已针对现有的实验数据进行了验证,其撞击速度高达约30kms -1。给出了插值方程,以预测直径在100nm至4μm之间,密度在2.4至7.8kg m -3的固体撞击器的坑深和直径。

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