We calculate phase transitions of uranium dioxide using structure factor in molecular dynamics. Our method is based on analysis of the rate of the structure factor change with the temperature. The temperatures of melting and transition to the superionic state for the uranium dioxide obtained by this method are 3100K and 2600K, respectively. Theses temperatures much better conform to the experimental values of 3120K and 2670K than in the radial distribution function analysis method. Other methods give the melting temperatures substantially higher (3435-3600K) than the experimental value.
Published in | International Journal of Materials Science and Applications (Volume 2, Issue 6) |
DOI | 10.11648/j.ijmsa.20130206.19 |
Page(s) | 228-232 |
Creative Commons |
This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited. |
Copyright |
Copyright © The Author(s), 2013. Published by Science Publishing Group |
Uranium Dioxide, Calculation of Phase Transitions, Rate of the Structure Factor Change, Molecular Dynamics
[1] | K. Govers, S. Lemehov, M. Hou, M. Verwerft "Comparison of interatomic potentials for UO2. Part I: Static calculations" in Journal of Nuclear Materials, Vol. 366, 2007, pp. 161–177. |
[2] | K. Govers, S. Lemehov, M. Hou, M. Verwerft "Comparison of interatomic potentials for UO2 Part II: Molecular dynamics simulations" in Journal of Nuclear Materials, Vol. 376, 2008, pp.66-77. |
[3] | C. Kittel, Introduction to solid state physics. Wiley, New York, 1971. |
[4] | S. Yamasaki, T. Arima, K. Idemitsu "Evalution of Thermal Conductivity Hyperstoihiometric UO2+x by Molecular Dynamics Simulation" in International Journal of Thermophysics, Vol.28, №2, 2007, pp.661-673. |
[5] | Agrawal1 P.M., Rice B.M., Thompson D.L. "Molecular dynamics study of the effects of voids and pressure in defect-nucleated melting simulations" in J. Chem. Phys., Vol. 118, 2003, pp.9680-9684. |
[6] | J. Solca, A. J. Dyson, G. Steinebrunner, B. Kirchner and H. Huber "Melting curves for neon calculated from pure theory" in J. Chem. Phys., Vol. 108, 1998, pp.4107-4111. |
[7] | D. G. Gromov, S. A. Gavrilov "Manifestation of the heterogeneous mechanism upon melting of low-dimensional systems" in Physics of the Solid State, Vol. 51, N 10, 2009. pp 2135-2144. |
[8] | C.B. Basak, A.K. Sengupta, H.S. Kamath "Classical molecular dynamics simulation of UO2 to predict thermophysical properties" in J. Alloys and Comp., Vol. 360, 2003, pp. 210-216. |
[9] | N.-D. Morelon, D. Ghaleb "A new empirical potential for simulating the formation of defects and their mobility in uranium dioxide" in Phil. Mag., Vol. 83, 2003, pp. 1533–1550. |
[10] | Yamada K., Kurosaki K., Uno M., Yamanaka S. Evaluation of thermal properties of uranium dioxide by molecular dynamics // J. Alloys and Comp. 2000. Vol. 307. P. 10-15. |
[11] | J.K. Fink "Thermophysical properties of uranium dioxide" in Journal of Nuclear Materials, Vol. 279, 2000, pp. 1-18. |
APA Style
Nagornov Yuri, Katz Andrey. (2013). Calculation of Phase Transitions of Uranium Dioxide Using Structure Factor in Molecular Dynamics. International Journal of Materials Science and Applications, 2(6), 228-232. https://doi.org/10.11648/j.ijmsa.20130206.19
ACS Style
Nagornov Yuri; Katz Andrey. Calculation of Phase Transitions of Uranium Dioxide Using Structure Factor in Molecular Dynamics. Int. J. Mater. Sci. Appl. 2013, 2(6), 228-232. doi: 10.11648/j.ijmsa.20130206.19
AMA Style
Nagornov Yuri, Katz Andrey. Calculation of Phase Transitions of Uranium Dioxide Using Structure Factor in Molecular Dynamics. Int J Mater Sci Appl. 2013;2(6):228-232. doi: 10.11648/j.ijmsa.20130206.19
@article{10.11648/j.ijmsa.20130206.19, author = {Nagornov Yuri and Katz Andrey}, title = {Calculation of Phase Transitions of Uranium Dioxide Using Structure Factor in Molecular Dynamics}, journal = {International Journal of Materials Science and Applications}, volume = {2}, number = {6}, pages = {228-232}, doi = {10.11648/j.ijmsa.20130206.19}, url = {https://doi.org/10.11648/j.ijmsa.20130206.19}, eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ijmsa.20130206.19}, abstract = {We calculate phase transitions of uranium dioxide using structure factor in molecular dynamics. Our method is based on analysis of the rate of the structure factor change with the temperature. The temperatures of melting and transition to the superionic state for the uranium dioxide obtained by this method are 3100K and 2600K, respectively. Theses temperatures much better conform to the experimental values of 3120K and 2670K than in the radial distribution function analysis method. Other methods give the melting temperatures substantially higher (3435-3600K) than the experimental value.}, year = {2013} }
TY - JOUR T1 - Calculation of Phase Transitions of Uranium Dioxide Using Structure Factor in Molecular Dynamics AU - Nagornov Yuri AU - Katz Andrey Y1 - 2013/12/30 PY - 2013 N1 - https://doi.org/10.11648/j.ijmsa.20130206.19 DO - 10.11648/j.ijmsa.20130206.19 T2 - International Journal of Materials Science and Applications JF - International Journal of Materials Science and Applications JO - International Journal of Materials Science and Applications SP - 228 EP - 232 PB - Science Publishing Group SN - 2327-2643 UR - https://doi.org/10.11648/j.ijmsa.20130206.19 AB - We calculate phase transitions of uranium dioxide using structure factor in molecular dynamics. Our method is based on analysis of the rate of the structure factor change with the temperature. The temperatures of melting and transition to the superionic state for the uranium dioxide obtained by this method are 3100K and 2600K, respectively. Theses temperatures much better conform to the experimental values of 3120K and 2670K than in the radial distribution function analysis method. Other methods give the melting temperatures substantially higher (3435-3600K) than the experimental value. VL - 2 IS - 6 ER -