Computer Simulation of Nickel and the Account for Electron Contributions in the Molecular Dynamics Method

Two new potentials are proposed for the embedded-atom model for nickel: one that includes the thermal contribution of electrons to the energy and one that disregards it. The potential parameters are found based on the nickel properties in isobar p = 0 and under shock compression with pressures up to...

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Veröffentlicht in:High temperature 2020, Vol.58 (1), p.64-77
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description Two new potentials are proposed for the embedded-atom model for nickel: one that includes the thermal contribution of electrons to the energy and one that disregards it. The potential parameters are found based on the nickel properties in isobar p = 0 and under shock compression with pressures up to ~760 GPa. The best consistency with experimental data is obtained when the electron contribution to the energy is taken into account. The calculated Hugoniot adiabat is in good agreement with the true curve. The inclusion of the electron contribution significantly reduces temperature on the adiabat and increases the cold pressure. The calculated melting curve of the nickel models gradually goes up to 4518 K at 300 GPa and is barely affected by the presence of the electron contribution. The coordinates of the melting section on the shock adiabat are determined (starting at 275.8 GPa and 4422 K and finishing at 297.6 GPa and 4499 K). The phase diagram of nickel with a stable bcc phase region at pressures above 110–130 GPa is proposed. Tables with the energies and pressures of the models at compression ratios up to 1.8182 are presented.
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The coordinates of the melting section on the shock adiabat are determined (starting at 275.8 GPa and 4422 K and finishing at 297.6 GPa and 4499 K). The phase diagram of nickel with a stable bcc phase region at pressures above 110–130 GPa is proposed. 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The calculated melting curve of the nickel models gradually goes up to 4518 K at 300 GPa and is barely affected by the presence of the electron contribution. The coordinates of the melting section on the shock adiabat are determined (starting at 275.8 GPa and 4422 K and finishing at 297.6 GPa and 4499 K). The phase diagram of nickel with a stable bcc phase region at pressures above 110–130 GPa is proposed. Tables with the energies and pressures of the models at compression ratios up to 1.8182 are presented.</description><subject>Atoms and Molecules in Strong Fields</subject><subject>Classical and Continuum Physics</subject><subject>Compression ratio</subject><subject>Computer simulation</subject><subject>Electrons</subject><subject>Embedded atom method</subject><subject>Industrial Chemistry/Chemical Engineering</subject><subject>Laser Matter Interaction</subject><subject>Materials Science</subject><subject>Molecular dynamics</subject><subject>Nickel</subject><subject>Phase diagrams</subject><subject>Physical Chemistry</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Thermophysical Properties of Materials</subject><issn>0018-151X</issn><issn>1608-3156</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNp1kM9LwzAYhoMoOKd_gLeA5-qXpOnqcdSfsOlhCt5KmiYus01mkh7235s6wYN4ygfv87yBF6FzApeEsPxqBUBKwskbTQcAyw_QhBRQZozw4hBNxjgb82N0EsIGADinbIJM5frtEJXHK9MPnYjGWew0fjLyQ3VY2BbHtcJzKd1gI9bO49tOyegTVjkbvWmG0QnY2G9y6VKcijy-2VnRGxnwUsW1a0_RkRZdUGc_7xS93t2-VA_Z4vn-sZovMslIETMuNS2ZpmqmyqLJdUm0gpbmkoMQJS1bophUEkgjgIFWekZmDWtIC9cMRNpiii72vVvvPgcVYr1xg7fpy5rmQDnwgueJIntKeheCV7reetMLv6sJ1OOi9Z9Fk0P3TkisfVf-t_l_6QthJHil</recordid><startdate>2020</startdate><enddate>2020</enddate><creator>Belashchenko, D. 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The best consistency with experimental data is obtained when the electron contribution to the energy is taken into account. The calculated Hugoniot adiabat is in good agreement with the true curve. The inclusion of the electron contribution significantly reduces temperature on the adiabat and increases the cold pressure. The calculated melting curve of the nickel models gradually goes up to 4518 K at 300 GPa and is barely affected by the presence of the electron contribution. The coordinates of the melting section on the shock adiabat are determined (starting at 275.8 GPa and 4422 K and finishing at 297.6 GPa and 4499 K). The phase diagram of nickel with a stable bcc phase region at pressures above 110–130 GPa is proposed. Tables with the energies and pressures of the models at compression ratios up to 1.8182 are presented.</abstract><cop>Moscow</cop><pub>Pleiades Publishing</pub><doi>10.1134/S0018151X20010034</doi><tpages>14</tpages></addata></record>
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subjects Atoms and Molecules in Strong Fields
Classical and Continuum Physics
Compression ratio
Computer simulation
Electrons
Embedded atom method
Industrial Chemistry/Chemical Engineering
Laser Matter Interaction
Materials Science
Molecular dynamics
Nickel
Phase diagrams
Physical Chemistry
Physics
Physics and Astronomy
Thermophysical Properties of Materials
title Computer Simulation of Nickel and the Account for Electron Contributions in the Molecular Dynamics Method
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