4.6 Article

Experimental and theoretical examination of shock-compressed copper through the fcc to bcc to melt phase transitions

Journal

JOURNAL OF APPLIED PHYSICS
Volume 132, Issue 7, Pages -

Publisher

AIP Publishing
DOI: 10.1063/5.0088607

Keywords

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Funding

  1. National Nuclear Security Administration [DE-NA0003902]
  2. NSF [1952923]
  3. U.S. Department of Energy (DOE)/National Nuclear Security Administration [DE-NA0003957]
  4. DOE Office of Science [DE-AC02-06CH11357]
  5. U.S. Department of Energy (DOE) by Lawrence Livermore National Laboratory under LLNL's Laboratory Directed Research and Development (LDRD) Program [18-ERD-001, 18-ERD-012, 21-ERD-032]
  6. U.S. Department of Energy, National Nuclear Security Administration [DE-AC52-07NA27344]
  7. Division Of Earth Sciences
  8. Directorate For Geosciences [1952923] Funding Source: National Science Foundation

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Recent studies have shown that several metals undergo a transformation from face-centered cubic (fcc) to body-centered cubic (bcc) structure during shock compression. Experiments and simulations have revealed that this fcc to bcc transition occurs at high pressures and temperatures, and the bcc structure remains stable at even higher pressures.
Recent studies show a face-centered cubic (fcc) to body-centered cubic (bcc) transformation along the shock Hugoniot for several metals (i.e., Cu, Au, and Ag). Here, we combine laser-shock compression of Cu foils on nanosecond timescales with in situ x-ray diffraction (XRD) to examine the microstructural changes with stress. We study the fcc phase and the phase transition from fcc to bcc (pressures greater than 180 GPa). Textural analysis of the azimuthal intensities from the XRD images is consistent with transformation into the bcc phase through the Pitsch-distortion mechanism. We use embedded atom model molecular dynamics simulations to determine the stability of the bcc phase in pressure-temperature space. Our results indicate that the bcc phase is stabilized only at high temperatures and remains stable at pressures greater than 500 GPa.

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