• Matter and Radiation at Extremes
  • Vol. 5, Issue 2, 28401 (2020)
N. J. Hartley1, C. Zhang2, X. Duan2, L. G. Huang1, S. Jiang2, Y. Li2, L. Yang3, A. Pelka4, Z. Wang2, J. Yang2, and D. Kraus5
Author Affiliations
  • 1Helmholtz-Zentrum Dresden-Rossendorf, 01328 Dresden, Germany
  • 2Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang, China
  • 3Helmholtz-Zentrum Dresden-Rossendorf, 01328 Dresden, Germany
  • 4Helmholtz-Zentrum Dresden-Rossendorf, 01328 Dresden, Germany
  • 5Helmholtz-Zentrum Dresden-Rossendorf, 01328 Dresden, Germany
  • show less
    DOI: 10.1063/1.5130726 Cite this Article
    N. J. Hartley, C. Zhang, X. Duan, L. G. Huang, S. Jiang, Y. Li, L. Yang, A. Pelka, Z. Wang, J. Yang, D. Kraus. Dynamically pre-compressed hydrocarbons studied by self-impedance mismatch[J]. Matter and Radiation at Extremes, 2020, 5(2): 28401 Copy Citation Text show less

    Abstract

    Using the SG-III prototype laser at China Academy of Engineering Physics, Mianyang, we irradiated polystyrene (CH) samples with a thermal radiation drive, reaching conditions on the principal Hugoniot up to P ≈ 1 TPa (10 Mbar), and away from the Hugoniot up to P ≈ 300 GPa (3 Mbar). The response of each sample was measured with a velocity interferometry diagnostic to determine the material and shock velocity, and hence the conditions reached, and the reflectivity of the sample, from which changes in the conductivity can be inferred. By applying the self-impedance mismatch technique with the measured velocities, the pressure and density of thermodynamic points away from the principal Hugoniot were determined. Our results show an unexpectedly large reflectivity at the highest shock pressures, while the off-Hugoniot points agree with previous work suggesting that shock-compressed CH conductivity is primarily temperature-dependent.
    P(up)=P1+ρ1(us,2up,1)(upup,1),(1)

    View in Article

    ρ2=ρ1us,2up,1us,2up,2.(2)

    View in Article

    uapp(t)=VPF×F(t)=n1up,1(n1n0)us,1,(3)

    View in Article

    uapp=(1.25×up,1)0.58,(4)

    View in Article

    uapp=n0us.(5)

    View in Article

    R=n2+iκn1n2+iκ+n12(6)

    View in Article

    =14n2n1(n2+n1)2+κ2,(7)

    View in Article

    N. J. Hartley, C. Zhang, X. Duan, L. G. Huang, S. Jiang, Y. Li, L. Yang, A. Pelka, Z. Wang, J. Yang, D. Kraus. Dynamically pre-compressed hydrocarbons studied by self-impedance mismatch[J]. Matter and Radiation at Extremes, 2020, 5(2): 28401
    Download Citation