Strength of tantalum to 276 GPa determined by two x-ray diffraction techniques using diamond anvil cells

Christopher Perreault, Larissa Q. Huston, Kaleb Burrage, Samantha C. Couper, Lowell Miyagi, Eric K. Moss, Jeffrey S. Pigott, Jesse S. Smith, Nenad Velisavljevic, Yogesh Vohra, Blake T. Sturtevant

Research output: Contribution to journalArticlepeer-review

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Abstract

Tantalum (Ta) is a metal that has useful properties that make it useful in extreme environments. It is, therefore, important to understand how Ta performs in such extreme conditions by accurately measuring its properties. In this work, the yield strength of tantalum has been measured at pressures up to 276 GPa using axial and radial x-ray diffraction (XRD) methods in diamond anvil cells (DACs). We measured strength using XRD in a radial DAC to 50 GPa, in an axial DAC to 60 GPa using diamonds with standard flat culets, and in a final experiment to 276 GPa using toroidal diamond anvils. The radial XRD data were refined using the Material Analysis Using Diffraction Rietveld software package to extract lattice strain and the yield strength. The axial data were refined using the General Structure Analysis System II and a linewidth method was used to calculate the yield strength. The yield strength measured near ambient pressure was found to be 0.5 GPa and increased with a pressure of up to 50 GPa, where the yield strength plateaued at a value of 2.4 GPa. At pressures above 60 GPa, the strength increased again to a maximum value of 9 GPa at the highest pressure of 276 GPa. The data from the three experiments show good agreement between the methods and previously reported experimental data. This agreement illustrates the value of axial diffraction data for material strength determination and allows for measurements at multi-hundreds of GPa using toroidal DACs.

Original languageEnglish
Article number015905
JournalJournal of Applied Physics
Volume131
Issue number1
DOIs
StatePublished - Jan 7 2022
Externally publishedYes

Funding

The research presented in this article was supported by the Laboratory Directed Research and Development program of Los Alamos National Laboratory (LANL), the G. T. Seaborg Institute under Laboratory Directed Research and Development (LDRD) (Project No. 20210527CR), and the LANL Office of Experimental Sciences, Dynamic Materials Properties Program. LANL is operated by Triad National Security, LLC for the DOE-NNSA under Contract No. 89233218CNA000001. Portions of this work were performed at HPCAT (Sector 16), Advanced Photon Source (APS), Argonne National Laboratory. HPCAT operations are supported by DOE-NNSA’s Office of Experimental Sciences. The Advanced Photon Source is a U.S. Department of Energy (DOE) Office of Science User Facility operated for the DOE Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357. Portions of this work were performed under the auspices of the U.S. Department of Energy by the Lawrence Livermore National Laboratory under Contract No. DE-AC52-07NA27344. We would like to acknowledge support from the U.S. National Science Foundation (NSF) under Metals and Metallic Nanostructures program (Grant No. DMR-1904164). We thank Saryu Fensin and George T. (Rusty) Gray III for their help with chemical characterization of the Ta sample used in the radial diffraction experiment. L.M. acknowledges support from US Department of Energy National Nuclear Security Administration through the Chicago-DOE Alliance Center (DE-NA0003975).

FundersFunder number
Chicago-DOE Alliance CenterDE-NA0003975
DOE-NNSA89233218CNA000001
DOE-NNSA’s Office of Experimental Sciences
G. T. Seaborg Institute20210527CR
National Science FoundationDMR-1904164
U.S. Department of Energy
Office of Science
National Nuclear Security Administration
Argonne National LaboratoryDE-AC02-06CH11357
Lawrence Livermore National LaboratoryDE-AC52-07NA27344
Laboratory Directed Research and Development
Los Alamos National Laboratory

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