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首页> 外文期刊>Journal of the European Ceramic Society >Static and dynamic indentation response of basal and prism plane sapphire
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Static and dynamic indentation response of basal and prism plane sapphire

机译:基面和棱镜平面蓝宝石的静态和动态压痕响应

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摘要

Static and dynamic indentation experiments are conducted on sapphire along the c[000 1] and a[1120] crystallographic axes to determine the loading rate dependence on its mechanical response. Static hardness is measured using a conventional Vickers tester while the dynamic hardness is measured using a custom test fixture based on split Hopkinson pressure bar technique with the capability to produce single indentations at strain rates of roughly 10~3 s~(-1). Static and dynamic hardness values as well as characteristic fracture response for both axes are compared at a range of indentation loads. The results indicate that dynamic hardness increases by 10% and 12% over static hardness for basal and prism plane sapphire, respectively. Observed crack orientations due to indentation of the a- and c-planes are consistent with the expected location of twinning or shp on the r(0 11 2), (110 2), (1012) and c(00 0 1) planes for both static and dynamic indentations. Prism slip is also suspected to interact with rhombohedral twinning systems to create a weakened zone oriented along the c-axis. Static indentations yielded well defined crystallographically oriented cracks with repeated directional switchbacks indicating a zone of competition between the two crack systems. Dynamic indentations, on the other hand, resulted in shorter and less jagged cracks accompanied by increased localized spalling beneath each indentation site as compared to the static indentations. This mode of fracture would suggest a shift in energy dissipation mechanism from crystal axis oriented long crack propagation under static loading to micro cracking that is independent of crystallographic orientation under higher strain rate events.
机译:在沿c [000 1]和a [1120]晶轴的蓝宝石上进行了静态和动态压痕实验,以确定加载速率取决于其机械响应。静态硬度是使用常规的维氏测试仪测量的,而动态硬度是使用基于拆分霍普金森压力棒技术的定制测试夹具测量的,该夹具能够以大约10〜3 s〜(-1)的应变速率产生单个压痕。在一定的压痕载荷范围内,比较了两个轴的静态和动态硬度值以及特征性的断裂响应。结果表明,相对于基底蓝宝石和棱镜面蓝宝石,动态硬度分别比静态硬度增加10%和12%。由于a平面和c平面的压痕而观察到的裂纹取向与r(0 11 2),(110 2),(1012)和c(00 0 1)平面上孪晶或shp的预期位置一致静态和动态缩进。还怀疑棱镜滑移会与菱形双晶孪晶系统相互作用,从而形成沿c轴定向的弱化区域。静态压痕产生了明确定义的晶体学取向的裂纹,并出现了反复的方向折返,表明这两个裂纹系统之间存在竞争区域。另一方面,与静态压痕相比,动态压痕导致较短和更少的锯齿状裂纹,并在每个压痕位置下方增加了局部剥落。这种断裂方式表明能量耗散机理从静态载荷下的晶轴定向长裂纹扩展转移到了独立于较高应变速率事件下的晶体学取向的微裂纹。

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