Molten uranium dioxide structure and dynamics

Author:

Skinner L. B.123,Benmore C. J.1,Weber J. K. R.13,Williamson M. A.4,Tamalonis A.1,Hebden A.4,Wiencek T.5,Alderman O. L. G.13,Guthrie M.6,Leibowitz L.4,Parise J. B.27

Affiliation:

1. X-ray Science Division, Argonne National Laboratory, Argonne, IL 60439, USA.

2. Mineral Physics Institute, Stony Brook University, Stony Brook, NY 11794-2100, USA.

3. Materials Development, Inc., 3090 Daniels Court, Arlington Heights, IL 60004, USA.

4. Chemical Science and Engineering, Argonne National Laboratory, Argonne, IL 60439, USA.

5. Nuclear Engineering, Argonne National Laboratory, Argonne, IL 60439, USA.

6. Geophysical Laboratory, Carnegie Institution of Washington, Washington, DC 20015, USA.

7. Photon Sciences, Brookhaven National Laboratory, Upton, NY 11973, USA

Abstract

Uranium dioxide (UO 2 ) is the major nuclear fuel component of fission power reactors. A key concern during severe accidents is the melting and leakage of radioactive UO 2 as it corrodes through its zirconium cladding and steel containment. Yet, the very high temperatures (>3140 kelvin) and chemical reactivity of molten UO 2 have prevented structural studies. In this work, we combine laser heating, sample levitation, and synchrotron x-rays to obtain pair distribution function measurements of hot solid and molten UO 2 . The hot solid shows a substantial increase in oxygen disorder around the lambda transition (2670 K) but negligible U-O coordination change. On melting, the average U-O coordination drops from 8 to 6.7 ± 0.5. Molecular dynamics models refined to this structure predict higher U-U mobility than 8-coordinated melts.

Publisher

American Association for the Advancement of Science (AAAS)

Subject

Multidisciplinary

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