不同尺度下不完善科尔斯基杆实验的有限元影响

Thomas H. Hannah, Reuben H. Kraft, V. Martin, Stephen Ellis
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引用次数: 0

摘要

典型的科尔斯基棒材直径为10-20mm,每个主棒材的长度以米为单位。为了推动104和更高的应变率,需要更小直径的棒材和更短的长度。随着杆的直径减小,系统的对准精度必须提高,以保持与较大的实验系统相同的相对公差。相反,随着杆的尺寸减小,由于系统质量减小,基于重力的摩擦力的大小也随之减小。有限元(FE)模型通常是假设一个完美的实验,具有精确的对准和无重力。此外,这些模拟倾向于利用理想实验的径向对称性,它消除了建模非对称效应的任何可能性,但具有减少计算负荷的附加好处。在这项工作中,我们讨论了这些快速运行的对称模型的一些结果,以建立一个基线,并展示了这些方法的一阶用例。然后,我们利用高性能计算技术生成几个三维,半对称模拟使用Abaqus®允许重力和不对准建模。缺陷最初使用静态一般过程建模,然后进行动态显式模拟,其中进行了试验的冲击部分。这种多步骤模拟结构创建了一个系统,可以正确地研究这些真实世界的非轴对称效果的影响。这些模拟充分探讨了这些实验现实的影响,并进行了详细描述,以允许其他研究人员实现类似的有限元建模结构,以帮助他们的实验和诊断工作。两个12.7毫米和3.16毫米直径棒系统进行评估,以量化的程度,这些不同的实验缺陷有跨科尔斯基棒系统的两个尺寸尺度。
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Impact of Imperfect Kolsky Bar Experiments Across Different Scales Using Finite Elements
Typical Kolsky bars are 10–20mm in diameter with the lengths of each main bar being on the scale of meters. To push 104 and higher strain rates smaller diameter bars, accompanied by shorter lengths, are needed. As the diameters of the bars decreases the precision in the alignment of the system must increase to maintain the same relative tolerance as the larger experimental systems. Conversely, as the size of the bars decreases so does the magnitude of gravity based frictional forces due to the decreased mass of the system. Finite Element (FE) models are typically generated assuming a perfect experiment with exact alignment and no gravity. Additionally, these simulations tend to take advantage of the radial symmetry of an ideal experiment which removes any potential for modeling non-symmetric effects but has the added benefit of a reduced computational load. In this work, we discuss some of the results of these fast-running symmetry models to establish a baseline and demonstrate the first-order use case of such methods. We then take advantage of high-performance computing techniques to generate several three-dimensional, half symmetry simulations using Abaqus® allowing modeling of gravity and misalignment. The imperfection is initially modeled using the static general process followed by a dynamic explicit simulation in which the impact portion of the test is conducted. This multi-step simulation structure creates a system that can properly investigate the impact of these real-world, non-axis symmetric effects. These simulations fully explore the impacts of these experimental realities and are described in detail to allow other researchers to implement a similar FE modeling structure to aid in their experimentation and diagnostic efforts. Both a 12.7 mm and 3.16 mm diameter bar system are evaluated to quantify the degree that these various experimental imperfections have across two size scales of Kolsky bar systems.
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