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Study on Titanium Alloy TC4 Ballistic Penetration Resistance Part Ⅰ: Ballistic Impact Tests

机译:钛合金TC4弹道抗穿透性研究第一部分:弹道冲击试验

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摘要

Ballistic impact test of different-scale casings is an efficient way to demonstrate the casing containment capability at the preliminary design stage of the engine.For the sake of studying the titanium alloy TC4 casing performance,the ballistic tests of flat and curved simulation casing are implemented by using two flat blades of different sizes as the projectile.The impact mechanism and failure of the target are discussed.Impact of the projectile is a highly nonlinear transient process with the large deformation of the target.On the impact,failures of the flat casing and the subscale casing are similar,concluding two parts,the global dishing and localized ductile tearing.The main localized failure mode combines plugging (shear) and petaling (shear) if the projectile perforates or penetrates,while crater (shear) if the projectile rebounds.The ballistic limit equation is verified by the test data and the results show that this empirical equation could be a practical way to estimate the critical velocity.
机译:在发动机的初步设计阶段,对不同尺度的壳体进行弹道冲击试验是证明其壳体密闭能力的有效方法。为了研究钛合金TC4壳体的性能,对平面和弯曲模拟壳体进行了弹道试验。通过使用两个不同大小的扁平叶片作为弹丸。讨论了靶的冲击机理和破坏。弹丸的影响是一个高度非线性的瞬态过程,靶的变形很大。在冲击上,扁平壳体的故障与局部尺度的壳体相似,包括整体凹陷和局部延性撕裂两部分。主要局部破坏模式是:如果射弹穿透或穿透,则堵塞(剪切)和成瓣(剪切),而如果弹丸反弹,则形成弹坑(剪切)。试验数据验证了弹道极限方程,结果表明该经验方程可能是估算弹道极限的实用方法。临界速度。

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  • 来源
    《中国航空学报(英文版)》 |2012年第3期|388-395|共8页
  • 作者单位

    College of Energy and Power Engineering,Nanjing University of Aeronautics and Astronautics,Nanjing 210016,China;

    College of Energy and Power Engineering,Nanjing University of Aeronautics and Astronautics,Nanjing 210016,China;

    College of Energy and Power Engineering,Nanjing University of Aeronautics and Astronautics,Nanjing 210016,China;

    College of Energy and Power Engineering,Nanjing University of Aeronautics and Astronautics,Nanjing 210016,China;

  • 收录信息 中国科学引文数据库(CSCD);中国科技论文与引文数据库(CSTPCD);
  • 原文格式 PDF
  • 正文语种 chi
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  • 入库时间 2024-01-27 04:24:19
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