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Temperature measurements in cerium shocked from 8.4 to 23.5 GPa

机译:铈中的温度测量从8.4触及8.4至23.5 gpa

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Shock temperature, stress, and dynamic emissivity for cerium shocked from 8.4 to 23.5 GPa were measured. In addition, the isentropic shock release temperature as a function of release stress was determined at a window interface. Cerium samples were shock compressed by plate impact on a single-stage gun. We made time-resolved measurements of thermal radiance, reflectance, and interface velocity of samples glued to lithium fluoride windows. Reflectance was measured with an integrating sphere and velocity with photonic Doppler velocimetry. From these measurements, we determined the temperature, emissivity, and stress at the interface. For shock stresses below 10.24 GPa, the samples were shocked from the γ phase into the α phase; at higher stresses, the cerium presumably melted or entered a mixed phase upon shock. The shock Hugoniot temperature as a function of stress follows a straight line over the entire range of our measurements, disagreeing with previously published predictions that the Hugoniot would follow the melt boundary from 10.24 up to around 16-18 GPa. Between 11.9 and 16.8 GPa, all the release isentropes converged (within experimental uncertainty) to a point around 4 GPa and 900 K, near the published melt curve. For experiments shocked above ~16GPa, the release isentropes behave differently. This suggests that within this 12-16 GPa range, there is a phase transition taking place, probably melt, and that it is occurring somewhere along the shock and release path. We could not identify a single-valued phase boundary from our experiments. Potential reasons for this are discussed.
机译:测量抗冲击温度,应力和动态发射率从8.4至23.5GPa震动。另外,在窗口界面中测定作为释放应力的函数的等熵冲击释放温度。铈样品被板撞击对单级枪的冲击压缩。我们在粘合到氟化锂窗口的样品的热辐射,反射率和界面速度的时间分辨测量。用积分球和光子多普勒速度测量反射率测量反射率。从这些测量中,我们确定了界面处的温度,发射率和应力。对于低于10.24GPa的冲击应力,将样品从γ相震动到α相中;在较高的应力下,铈可能在休克时熔化或进入混合相。随着压力的函数的冲击Hugoniot温度遵循整个测量范围的直线,不同意先前公布的预测,即Hugoniot将从10.24到大约16-18 GPA的熔体边界遵循熔体边界。在11.9和16.8GPa之间,所有释放等熵在公开的熔体曲线附近收敛(在实验性不确定性内)到大约4GPa和900 k的点。对于实验令人震惊〜16GPa,释放等熵表现不同。这表明在该12-16 GPA范围内,可能发生了相变,可能熔化,并且它在沿着震动和释放路径的某处发生。我们无法从我们的实验中识别单值相位边界。讨论了潜在原因。

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  • 来源
    《Journal of Applied Physics》 |2021年第15期|155106.1-155106.11|共11页
  • 作者单位

    Nevada National Security Site Transformational Diagnostics and Imaging Los Alamos New Mexico 87544 USA;

    Nevada National Security Site Special Technologies Laboratory Santa Barbara California 93111 USA;

    Nevada National Security Site Special Technologies Laboratory Santa Barbara California 93111 USA;

    Nevada National Security Site Special Technologies Laboratory Santa Barbara California 93111 USA;

    Nevada National Security Site Special Technologies Laboratory Santa Barbara California 93111 USA;

    Nevada National Security Site Transformational Diagnostics and Imaging Los Alamos New Mexico 87544 USA Nevada National Security Site Special Technologies Laboratory Santa Barbara California 93111 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);
  • 原文格式 PDF
  • 正文语种 eng
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