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Understanding the evolution of liquid and solid microjets from grooved Sn and Cu samples using radiography

机译:使用射线照相从槽Sn和Cu样品中了解液体和固体微颈喷裂样的演变

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摘要

Experiments were performed on grooved Sn and Cu samples to study the temporal evolution of microjets. Jets were generated by the impact of gun-launched flyer plates against the back of grooved targets made from either Cu or Sn (groove depth of ~250μm). The Hugoniot states in the various Sn targets encompassed conditions where solid phases are maintained throughout (7 and 16 GPa) and also conditions where melting occurs upon the release of compression (25 and 34 GPa); the transition occurs near a Hugoniot pressure of 23 GPa. Cu targets at 27 and 56 GPa provide comparisons in which the jets move at similar speeds but remain solid. In all cases, the spatial distribution of mass within the microjets was measured using high-speed synchrotron radiography. The result is a time history of the jet thickness profile from which quantities like total jet mass and jet velocity can be derived. In both the solid and liquid states, we generally observe that an increase in the shock strength leads to an increase in jet mass. However, this trend breaks down for Hugoniot states near the transition from continuously solid to melted-on-release. This is evidenced by the observation that there was no difference in the rate of mass flow in Sn jets at 16 and 25 GPa, while similar pressure jumps on either side of this range caused substantial changes in the jet mass. This contrasts with the behavior of smaller polishing defects that were present on the same samples (~1μm deep). From these, no ejecta mass was detected below the melt boundary, but obvious microjets were generated once melting occurred. This indicates that crossing the bulk melt-on-release threshold can alternately promote or inhibit the flow of mass into microjets based on the amplitude of the initial perturbation.
机译:在槽Sn和Cu样品上进行实验,以研究微目亡的时间演变。喷枪由枪发射的传单板对由Cu或Sn(槽深的〜250μm)制成的凹槽靶背面的影响产生。 Hugoniot在各种Sn靶中包含固体相保持(7和16GPa)的条件,以及在释放压缩时发生熔化的条件(25和34GPa);过渡发生在23 GPa的Hugoniot压力附近。 27和56 GPA的Cu靶标提供比较,其中喷射器以类似的速度移动,但保持稳定。在所有情况下,使用高速同步辐射照相术测量微目词内的质量的空间分布。结果是喷射厚度曲线的时间历史,其可以推导出总喷射质量和喷射速度的量。在固体和液体状态的两种情况下,我们通常观察到震荡强度的增加导致喷射质量的增加。然而,这种趋势对于Hugoniot州附近的过渡到融合释放的过渡附近。这是通过观察所证明的,即在16和25GPa的Sn喷射中的质量流量率没有差异,而该范围两侧的类似压力跳跃导致喷射质量的显着变化。这与存在于相同样品(〜1μm深)上存在的较小抛光缺陷的行为形成鲜明对比。由此,在熔体边界下方未检测到喷射物质量,但一旦发生熔化,产生明显的微进口。这表明通过初始扰动的幅度交替地促进或抑制大量熔体释放阈值,可以替代地促进或抑制物质的流量。

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  • 来源
    《Journal of Applied Physics》 |2021年第4期|045901.1-045901.12|共12页
  • 作者单位

    Lawrence Livermore National Laboratory Livermore California 94550 USA;

    Lawrence Livermore National Laboratory Livermore California 94550 USA;

    Lawrence Livermore National Laboratory Livermore California 94550 USA;

    Lawrence Livermore National Laboratory Livermore California 94550 USA;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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  • 正文语种 eng
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