Effects of EOS and constitutive models on simulating copper shaped charge jets in ALEGRA

R. Doney, J. Niederhaus, T. Fuller, M. Coppinger
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Abstract

Metallic shaped charge jets (SCJ) have been studied for many decades across multiple communities for applications ranging from military warheads to earth penetrators for accessing oil-rich areas [1]. Researchers have had varied success in modeling these jets using simulation codes such as CTH, ALEGRA, and ALE3D. Recently, a large amount of work has been performed at the US Army Research Lab investigating the behavior of jets with increasingly sophisticated experimental diagnostics. Advances in computational resources, code enhancements, and material models have allowed us to model jets and probe uncertainties caused by algorithms, equations of state (EOS), constitutive models, and any of the available parameters each one provides. In this work we explore the effects that various EOS and constitutive models have on the development and characteristics of a 65-mm diameter, 2D copper SCJ using the Sandia National Laboratories’ multiphysics hydrocode, ALEGRA [2]. Specifically, we evaluate the tabular SESAME 3320 [3], 3325 [4-5], and 3337 [6] EOS models, analytic EOS (ANEOS) 3331 [7], as well as the Johnson-Cook (JC) [8], Zerilli-Armstrong (ZA) [9], Preston-Tonks-Wallace (PTW) [10], Steinberg-Guinan-Lund (SGL) [11-12], and Mechanical Threshold Stress (MTS) [13] constitutive models. Note that while the SGL model supports rate-dependence, there is no current characterization for copper, thus we are using rate-independent version. We do not consider the MieGrüneisen equation of state here as we expect parts of the jet to be near or cross into melt.
EOS和本构模型对ALEGRA中铜聚能射流模拟的影响
金属聚能射流(SCJ)已经在多个领域进行了数十年的研究,其应用范围从军用弹头到进入富油区的地球穿透器。研究人员使用CTH、ALEGRA和ALE3D等模拟代码对这些喷气机进行建模,取得了不同程度的成功。最近,美国陆军研究实验室进行了大量的工作,用越来越复杂的实验诊断来调查喷气机的行为。计算资源、代码增强和材料模型的进步使我们能够对射流进行建模,并探测由算法、状态方程(EOS)、本构模型和每个模型提供的任何可用参数引起的不确定性。在这项工作中,我们使用桑迪亚国家实验室的多物理场氢代码ALEGRA[2]探索了各种EOS和本构模型对65毫米直径2D铜SCJ的发展和特性的影响。具体而言,我们评估了表格式SESAME 3320[3]、3325[4-5]和3337 [6]EOS模型、解析式EOS (ANEOS) 3331[7],以及Johnson-Cook (JC)[8]、zerillii - armstrong (ZA)[9]、Preston-Tonks-Wallace (PTW)[10]、steinberg - guinian - lund (SGL)[11-12]和机械阈值应力(MTS)[13]本构模型。请注意,虽然SGL模型支持速率依赖,但目前还没有铜的特性描述,因此我们使用的是速率无关的版本。我们在这里不考虑米格-格- 尼森状态方程,因为我们预计射流的部分会接近或交叉进入熔体。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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