Prediction of Second Melting Temperatures Already Observed in Pure Elements by Molecular Dynamics Simulations

A second melting temperature occurs at a temperature T<sub>n+</sub> higher than T<sub>m</sub> in glass-forming melts after heating them from their glassy state. The melting entropy is reduced or increased depending on the thermal history and on the presence of antibonds or bo...

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Autores principales: Robert F. Tournier, Michael I. Ojovan
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spelling oai:doaj.org-article:36ff50ba67b041c4b09f5964a22eb8bb2021-11-11T18:04:49ZPrediction of Second Melting Temperatures Already Observed in Pure Elements by Molecular Dynamics Simulations10.3390/ma142165091996-1944https://doaj.org/article/36ff50ba67b041c4b09f5964a22eb8bb2021-10-01T00:00:00Zhttps://www.mdpi.com/1996-1944/14/21/6509https://doaj.org/toc/1996-1944A second melting temperature occurs at a temperature T<sub>n+</sub> higher than T<sub>m</sub> in glass-forming melts after heating them from their glassy state. The melting entropy is reduced or increased depending on the thermal history and on the presence of antibonds or bonds up to T<sub>n+</sub>. Recent MD simulations show full melting at T<sub>n+</sub> = 1.119T<sub>m</sub> for Zr, 1.126T<sub>m</sub> for Ag, 1.219T<sub>m</sub> for Fe and 1.354T<sub>m</sub> for Cu. The non-classical homogeneous nucleation model applied to liquid elements is based on the increase of the Lindemann coefficient with the heating rate. The glass transition at T<sub>g</sub> and the nucleation temperatures T<sub>nG</sub> of glacial phases are successfully predicted below and above T<sub>m</sub>. The glass transition temperature T<sub>g</sub> increases with the heating rate up to T<sub>n+</sub>. Melting and crystallization of glacial phases occur with entropy and enthalpy reductions. A universal law relating T<sub>n+</sub> and T<sub>nG</sub> around T<sub>m</sub> shows that T<sub>nG</sub> cannot be higher than 1.293T<sub>m</sub> for T<sub>n+</sub>= 1.47T<sub>m</sub>. The enthalpies and entropies of glacial phases have singular values, corresponding to the increase of percolation thresholds with T<sub>g</sub> and T<sub>nG</sub> above the Scher and Zallen invariant at various heating and cooling rates. The G-phases are metastable up to T<sub>n+</sub> because the antibonds are broken by homogeneous nucleation of bonds.Robert F. TournierMichael I. OjovanMDPI AGarticlemelting enthalpy and entropysecond melting temperaturemelting entropy reductioncrystallization enthalpy reductionundercoolingoverheatingTechnologyTElectrical engineering. Electronics. Nuclear engineeringTK1-9971Engineering (General). Civil engineering (General)TA1-2040MicroscopyQH201-278.5Descriptive and experimental mechanicsQC120-168.85ENMaterials, Vol 14, Iss 6509, p 6509 (2021)
institution DOAJ
collection DOAJ
language EN
topic melting enthalpy and entropy
second melting temperature
melting entropy reduction
crystallization enthalpy reduction
undercooling
overheating
Technology
T
Electrical engineering. Electronics. Nuclear engineering
TK1-9971
Engineering (General). Civil engineering (General)
TA1-2040
Microscopy
QH201-278.5
Descriptive and experimental mechanics
QC120-168.85
spellingShingle melting enthalpy and entropy
second melting temperature
melting entropy reduction
crystallization enthalpy reduction
undercooling
overheating
Technology
T
Electrical engineering. Electronics. Nuclear engineering
TK1-9971
Engineering (General). Civil engineering (General)
TA1-2040
Microscopy
QH201-278.5
Descriptive and experimental mechanics
QC120-168.85
Robert F. Tournier
Michael I. Ojovan
Prediction of Second Melting Temperatures Already Observed in Pure Elements by Molecular Dynamics Simulations
description A second melting temperature occurs at a temperature T<sub>n+</sub> higher than T<sub>m</sub> in glass-forming melts after heating them from their glassy state. The melting entropy is reduced or increased depending on the thermal history and on the presence of antibonds or bonds up to T<sub>n+</sub>. Recent MD simulations show full melting at T<sub>n+</sub> = 1.119T<sub>m</sub> for Zr, 1.126T<sub>m</sub> for Ag, 1.219T<sub>m</sub> for Fe and 1.354T<sub>m</sub> for Cu. The non-classical homogeneous nucleation model applied to liquid elements is based on the increase of the Lindemann coefficient with the heating rate. The glass transition at T<sub>g</sub> and the nucleation temperatures T<sub>nG</sub> of glacial phases are successfully predicted below and above T<sub>m</sub>. The glass transition temperature T<sub>g</sub> increases with the heating rate up to T<sub>n+</sub>. Melting and crystallization of glacial phases occur with entropy and enthalpy reductions. A universal law relating T<sub>n+</sub> and T<sub>nG</sub> around T<sub>m</sub> shows that T<sub>nG</sub> cannot be higher than 1.293T<sub>m</sub> for T<sub>n+</sub>= 1.47T<sub>m</sub>. The enthalpies and entropies of glacial phases have singular values, corresponding to the increase of percolation thresholds with T<sub>g</sub> and T<sub>nG</sub> above the Scher and Zallen invariant at various heating and cooling rates. The G-phases are metastable up to T<sub>n+</sub> because the antibonds are broken by homogeneous nucleation of bonds.
format article
author Robert F. Tournier
Michael I. Ojovan
author_facet Robert F. Tournier
Michael I. Ojovan
author_sort Robert F. Tournier
title Prediction of Second Melting Temperatures Already Observed in Pure Elements by Molecular Dynamics Simulations
title_short Prediction of Second Melting Temperatures Already Observed in Pure Elements by Molecular Dynamics Simulations
title_full Prediction of Second Melting Temperatures Already Observed in Pure Elements by Molecular Dynamics Simulations
title_fullStr Prediction of Second Melting Temperatures Already Observed in Pure Elements by Molecular Dynamics Simulations
title_full_unstemmed Prediction of Second Melting Temperatures Already Observed in Pure Elements by Molecular Dynamics Simulations
title_sort prediction of second melting temperatures already observed in pure elements by molecular dynamics simulations
publisher MDPI AG
publishDate 2021
url https://doaj.org/article/36ff50ba67b041c4b09f5964a22eb8bb
work_keys_str_mv AT robertftournier predictionofsecondmeltingtemperaturesalreadyobservedinpureelementsbymoleculardynamicssimulations
AT michaeliojovan predictionofsecondmeltingtemperaturesalreadyobservedinpureelementsbymoleculardynamicssimulations
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