Your browser doesn't support javascript.
loading
Melting of Tantalum at Multimegabar Pressures on the Nanosecond Timescale.
Kraus, R G; Coppari, F; Fratanduono, D E; Smith, R F; Lazicki, A; Wehrenberg, C; Eggert, J H; Rygg, J R; Collins, G W.
Afiliação
  • Kraus RG; Physics Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
  • Coppari F; Physics Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
  • Fratanduono DE; Physics Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
  • Smith RF; Physics Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
  • Lazicki A; Physics Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
  • Wehrenberg C; Physics Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
  • Eggert JH; Physics Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
  • Rygg JR; Laboratory for Laser Energetics, and Departments of Mechanical Engineering and Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA.
  • Collins GW; Laboratory for Laser Energetics, and Departments of Mechanical Engineering and Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA.
Phys Rev Lett ; 126(25): 255701, 2021 Jun 25.
Article em En | MEDLINE | ID: mdl-34241515
Tantalum was once thought to be the canonical bcc metal, but is now predicted to transition to the Pnma phase at the high pressures and temperatures expected along the principal Hugoniot. Furthermore, there remains a significant discrepancy between a number of static diamond anvil cell experiments and gas gun experiments in the measured melt temperatures at high pressures. Our in situ x-ray diffraction experiments on shock compressed tantalum show that it does not transition to the Pnma phase or other candidate phases at high pressure. We observe incipient melting at approximately 254±15 GPa and complete melting by 317±10 GPa. These transition pressures from the nanosecond experiments presented here are consistent with what can be inferred from microsecond gas gun sound velocity measurements. Furthermore, the observation of a coexistence region on the Hugoniot implies the lack of significant kinetically controlled deviation from equilibrium behavior. Consequently, we find that kinetics of phase transitions cannot be used to explain the discrepancy between static and dynamic measurements of the tantalum melt curve. Using available high pressure thermodynamic data for tantalum and our measurements of the incipient and complete melting transition pressures, we are able to infer a melting temperature 8070_{-750}^{+1250} K at 254±15 GPa, which is consistent with ambient and a recent static high pressure melt curve measurement.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2021 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2021 Tipo de documento: Article