High-precision molecular dynamics simulation of UO2aPuO2: Anion self-diffusion in UO2
Our series of articles is devoted to high-precision molecular dynamics simulation of mixed actinide-oxide (MOX) fuel in the approximation of rigid ions and pair interactions (RIPI) using high-performance graphics processors (GPU). In this article we study self-diffusion mechanisms of oxygen anions i...
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Veröffentlicht in: | Journal of nuclear materials 2013-02, Vol.433 (1-3), p.215-226 |
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creator | Potashnikov, SI Boyarchenkov, A S Nekrasov, KA Kupryazhkin, AYa |
description | Our series of articles is devoted to high-precision molecular dynamics simulation of mixed actinide-oxide (MOX) fuel in the approximation of rigid ions and pair interactions (RIPI) using high-performance graphics processors (GPU). In this article we study self-diffusion mechanisms of oxygen anions in uranium dioxide (UO2) with the 10 recent and widely used sets of interatomic pair potentials (SPP) under periodic (PBC) and isolated (IBC) boundary conditions. Wide range of measured diffusion coefficients (from 10-3 cm2/s at melting point down to 10-12 cm2/s at 1400 K) made possible a direct comparison (without extrapolation) of the simulation results with the experimental data, which have been known only at low temperatures (T < 1500 K). A highly detailed (with the temperature step of 1 K) calculation of the diffusion coefficient allowed us to plot temperature dependences of the diffusion activation energy and its derivative, both of which show a wide ( similar to 1000 K) superionic transition region confirming the broad I>-peaks of heat capacity obtained by us earlier. It is shown that regardless of SPP the anion self-diffusion in model crystals without surface or artificially embedded defects goes on via exchange mechanism, rather than interstitial or vacancy mechanisms suggested by the previous works. The activation energy of exchange diffusion turned out to coincide with the anti-Frenkel defect formation energy calculated by the lattice statics. |
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In this article we study self-diffusion mechanisms of oxygen anions in uranium dioxide (UO2) with the 10 recent and widely used sets of interatomic pair potentials (SPP) under periodic (PBC) and isolated (IBC) boundary conditions. Wide range of measured diffusion coefficients (from 10-3 cm2/s at melting point down to 10-12 cm2/s at 1400 K) made possible a direct comparison (without extrapolation) of the simulation results with the experimental data, which have been known only at low temperatures (T < 1500 K). A highly detailed (with the temperature step of 1 K) calculation of the diffusion coefficient allowed us to plot temperature dependences of the diffusion activation energy and its derivative, both of which show a wide ( similar to 1000 K) superionic transition region confirming the broad I>-peaks of heat capacity obtained by us earlier. It is shown that regardless of SPP the anion self-diffusion in model crystals without surface or artificially embedded defects goes on via exchange mechanism, rather than interstitial or vacancy mechanisms suggested by the previous works. 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In this article we study self-diffusion mechanisms of oxygen anions in uranium dioxide (UO2) with the 10 recent and widely used sets of interatomic pair potentials (SPP) under periodic (PBC) and isolated (IBC) boundary conditions. Wide range of measured diffusion coefficients (from 10-3 cm2/s at melting point down to 10-12 cm2/s at 1400 K) made possible a direct comparison (without extrapolation) of the simulation results with the experimental data, which have been known only at low temperatures (T < 1500 K). A highly detailed (with the temperature step of 1 K) calculation of the diffusion coefficient allowed us to plot temperature dependences of the diffusion activation energy and its derivative, both of which show a wide ( similar to 1000 K) superionic transition region confirming the broad I>-peaks of heat capacity obtained by us earlier. It is shown that regardless of SPP the anion self-diffusion in model crystals without surface or artificially embedded defects goes on via exchange mechanism, rather than interstitial or vacancy mechanisms suggested by the previous works. The activation energy of exchange diffusion turned out to coincide with the anti-Frenkel defect formation energy calculated by the lattice statics.</description><subject>Activation energy</subject><subject>Anions</subject><subject>Crystal defects</subject><subject>Diffusion</subject><subject>Diffusion coefficient</subject><subject>Mathematical models</subject><subject>Molecular dynamics</subject><subject>Simulation</subject><issn>0022-3115</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><recordid>eNqVjbsKwjAYhTMoWC_vkNGlkKSkUDcRpVsd7CwhTfSXXLR_M_j2tuILOB34znc4M5IxJkRecC4XZIn4YIzJismMtDXc7vmzNxoQYqA-OqOTUz3t3kF50EgR_AiGqY2Wto1Q59SIHd2HCaFxNu_A2vTdQ5iMNZlb5dBsfrki29PxcqjHo_hKBoerB9TGORVMTHjlRSk5r3jJij_UD6ovQ1E</recordid><startdate>20130201</startdate><enddate>20130201</enddate><creator>Potashnikov, SI</creator><creator>Boyarchenkov, A S</creator><creator>Nekrasov, KA</creator><creator>Kupryazhkin, AYa</creator><scope>7SR</scope><scope>7TB</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>FR3</scope><scope>H8D</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20130201</creationdate><title>High-precision molecular dynamics simulation of UO2aPuO2: Anion self-diffusion in UO2</title><author>Potashnikov, SI ; Boyarchenkov, A S ; Nekrasov, KA ; Kupryazhkin, AYa</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_miscellaneous_13651191603</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>Activation energy</topic><topic>Anions</topic><topic>Crystal defects</topic><topic>Diffusion</topic><topic>Diffusion coefficient</topic><topic>Mathematical models</topic><topic>Molecular dynamics</topic><topic>Simulation</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Potashnikov, SI</creatorcontrib><creatorcontrib>Boyarchenkov, A S</creatorcontrib><creatorcontrib>Nekrasov, KA</creatorcontrib><creatorcontrib>Kupryazhkin, AYa</creatorcontrib><collection>Engineered Materials Abstracts</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of nuclear materials</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Potashnikov, SI</au><au>Boyarchenkov, A S</au><au>Nekrasov, KA</au><au>Kupryazhkin, AYa</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>High-precision molecular dynamics simulation of UO2aPuO2: Anion self-diffusion in UO2</atitle><jtitle>Journal of nuclear materials</jtitle><date>2013-02-01</date><risdate>2013</risdate><volume>433</volume><issue>1-3</issue><spage>215</spage><epage>226</epage><pages>215-226</pages><issn>0022-3115</issn><abstract>Our series of articles is devoted to high-precision molecular dynamics simulation of mixed actinide-oxide (MOX) fuel in the approximation of rigid ions and pair interactions (RIPI) using high-performance graphics processors (GPU). In this article we study self-diffusion mechanisms of oxygen anions in uranium dioxide (UO2) with the 10 recent and widely used sets of interatomic pair potentials (SPP) under periodic (PBC) and isolated (IBC) boundary conditions. Wide range of measured diffusion coefficients (from 10-3 cm2/s at melting point down to 10-12 cm2/s at 1400 K) made possible a direct comparison (without extrapolation) of the simulation results with the experimental data, which have been known only at low temperatures (T < 1500 K). A highly detailed (with the temperature step of 1 K) calculation of the diffusion coefficient allowed us to plot temperature dependences of the diffusion activation energy and its derivative, both of which show a wide ( similar to 1000 K) superionic transition region confirming the broad I>-peaks of heat capacity obtained by us earlier. It is shown that regardless of SPP the anion self-diffusion in model crystals without surface or artificially embedded defects goes on via exchange mechanism, rather than interstitial or vacancy mechanisms suggested by the previous works. The activation energy of exchange diffusion turned out to coincide with the anti-Frenkel defect formation energy calculated by the lattice statics.</abstract></addata></record> |
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subjects | Activation energy Anions Crystal defects Diffusion Diffusion coefficient Mathematical models Molecular dynamics Simulation |
title | High-precision molecular dynamics simulation of UO2aPuO2: Anion self-diffusion in UO2 |
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