弹塑性环境中弱变形体的耦合计算及变形模态的定义

A. А. Krayukhin, V. V. Borlyaev, M. V. Skobeeva, A. Stadnik
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引用次数: 0

摘要

本文提出了一种对弹塑性环境中运动的弱变形体进行耦合模拟并确定其变形模式的技术。弹丸的侵彻计算是用EGAK法在固定计算网格上进行的,这意味着弹丸是刚性的,其内部结构不重要。流体流动在与静止弹丸相连的非惯性基座中计算(使用BODY-3D方法)。利用软件LOGOS,在拉格朗日网格上计算了弹丸的变形模式。采用符合要求的弹体细部有限元模型,并结合弹体结构件的弹塑性材料特性进行分析。弹丸的加载是通过在弹丸的外表面分配力边界条件来实现的。给出了耦合计算方法和试验结果。本文的实验结果表明,采用该技术得到的试验结果与在固定计算网格上直接建模的结果吻合较好。以MoonLITE探地雷达侵入软土屏障为例,给出了该技术的计算结果。该穿透器是在月球研究任务MoonLITE的范围内开发的,可以深入月球土壤。数值模拟结果与实验数据吻合较好,平均减速率最大差异为10-15%。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
COUPLED CALCULATIONS OF WEAKLY DEFORMABLE BODIES MOVING IN ELASTOPLASTIC ENVIRONMENT AND DEFINING ITS MODE OF DEFORMATION
This paper presents a technology of making coupled simulations of weakly deformable bodies moving in elastoplastic environment and defining its mode of deformation. Calculation of penetration of a projectile is made by EGAK methods on a fixed calculating mesh implying that the projectile is rigid and its inner structure is unimportant. Fluid flow is calculated in a noninertial base that is connected with the stationary projectile (using BODY-3D method). Mode of deformation of the projectile is calculated on a Lagrangian mesh using software package LOGOS. Finite-element model of the projectile with the required degree of detail is used with real elastoplastic material properties of its structural parts. Loading of the projectile is implemented with an assignment of force boundary condition on its outer surface. Methods of coupling calculations and test results are provided. In this paper, it is shown that test results obtained by this developed technology are in a good agreement with direct modeling on a fixed calculating mesh. As an example of using this technology, calculation results of a penetrator-probe MoonLITE intruding into a soft soil barrier are presented. This penetrator is developed within the scope of MoonLITE mission of studying the Moon and can deepen into moon soil. Results of numerical simulations are in a good agreement with the experimental data, maximum difference for average slow-down rate of the penetrator is 10–15%.
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