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First-Principles Structural, Mechanical, and Thermodynamic Calculations of the Negative Thermal Expansion Compound Zr(2)(WO(4))(PO(4))(2)
[Image: see text] The negative thermal expansion (NTE) material Zr(2)(WO(4))(PO(4))(2) has been investigated for the first time within the framework of the density functional perturbation theory (DFPT). The structural, mechanical, and thermodynamic properties of this material have been predicted usi...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2018
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6644104/ https://www.ncbi.nlm.nih.gov/pubmed/31458228 http://dx.doi.org/10.1021/acsomega.8b02456 |
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author | Weck, Philippe F. Kim, Eunja Gordon, Margaret E. Greathouse, Jeffery A. Dingreville, Rémi Bryan, Charles R. |
author_facet | Weck, Philippe F. Kim, Eunja Gordon, Margaret E. Greathouse, Jeffery A. Dingreville, Rémi Bryan, Charles R. |
author_sort | Weck, Philippe F. |
collection | PubMed |
description | [Image: see text] The negative thermal expansion (NTE) material Zr(2)(WO(4))(PO(4))(2) has been investigated for the first time within the framework of the density functional perturbation theory (DFPT). The structural, mechanical, and thermodynamic properties of this material have been predicted using the Perdew, Burke and Ernzerhof for solid (PBEsol) exchange–correlation functional, which showed superior accuracy over standard functionals in previous computational studies of the NTE material α-ZrW(2)O(8). The bulk modulus calculated for Zr(2)(WO(4))(PO(4))(2) using the Vinet equation of state at room temperature is K(0) = 63.6 GPa, which is in close agreement with the experimental estimate of 61.3(8) at T = 296 K. The computed mean linear coefficient of thermal expansion is −3.1 × 10(–6) K(−1) in the temperature range ∼0–70 K, in line with the X-ray diffraction measurements. The mean Grüneisen parameter controlling the thermal expansion of Zr(2)(WO(4))(PO(4))(2) is negative below 205 K, with a minimum of −2.1 at 10 K. The calculated standard molar heat capacity and entropy are C(P)(0) = 287.6 and S(0) = 321.9 J·mol(–1)·K(–1), respectively. The results reported in this study demonstrate the accuracy of DFPT/PBEsol for assessing or predicting the relationship between structural and thermomechanical properties of NTE materials. |
format | Online Article Text |
id | pubmed-6644104 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2018 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-66441042019-08-27 First-Principles Structural, Mechanical, and Thermodynamic Calculations of the Negative Thermal Expansion Compound Zr(2)(WO(4))(PO(4))(2) Weck, Philippe F. Kim, Eunja Gordon, Margaret E. Greathouse, Jeffery A. Dingreville, Rémi Bryan, Charles R. ACS Omega [Image: see text] The negative thermal expansion (NTE) material Zr(2)(WO(4))(PO(4))(2) has been investigated for the first time within the framework of the density functional perturbation theory (DFPT). The structural, mechanical, and thermodynamic properties of this material have been predicted using the Perdew, Burke and Ernzerhof for solid (PBEsol) exchange–correlation functional, which showed superior accuracy over standard functionals in previous computational studies of the NTE material α-ZrW(2)O(8). The bulk modulus calculated for Zr(2)(WO(4))(PO(4))(2) using the Vinet equation of state at room temperature is K(0) = 63.6 GPa, which is in close agreement with the experimental estimate of 61.3(8) at T = 296 K. The computed mean linear coefficient of thermal expansion is −3.1 × 10(–6) K(−1) in the temperature range ∼0–70 K, in line with the X-ray diffraction measurements. The mean Grüneisen parameter controlling the thermal expansion of Zr(2)(WO(4))(PO(4))(2) is negative below 205 K, with a minimum of −2.1 at 10 K. The calculated standard molar heat capacity and entropy are C(P)(0) = 287.6 and S(0) = 321.9 J·mol(–1)·K(–1), respectively. The results reported in this study demonstrate the accuracy of DFPT/PBEsol for assessing or predicting the relationship between structural and thermomechanical properties of NTE materials. American Chemical Society 2018-11-20 /pmc/articles/PMC6644104/ /pubmed/31458228 http://dx.doi.org/10.1021/acsomega.8b02456 Text en Copyright © 2018 American Chemical Society This is an open access article published under an ACS AuthorChoice License (http://pubs.acs.org/page/policy/authorchoice_termsofuse.html) , which permits copying and redistribution of the article or any adaptations for non-commercial purposes. |
spellingShingle | Weck, Philippe F. Kim, Eunja Gordon, Margaret E. Greathouse, Jeffery A. Dingreville, Rémi Bryan, Charles R. First-Principles Structural, Mechanical, and Thermodynamic Calculations of the Negative Thermal Expansion Compound Zr(2)(WO(4))(PO(4))(2) |
title | First-Principles Structural, Mechanical, and Thermodynamic
Calculations of the Negative Thermal Expansion Compound Zr(2)(WO(4))(PO(4))(2) |
title_full | First-Principles Structural, Mechanical, and Thermodynamic
Calculations of the Negative Thermal Expansion Compound Zr(2)(WO(4))(PO(4))(2) |
title_fullStr | First-Principles Structural, Mechanical, and Thermodynamic
Calculations of the Negative Thermal Expansion Compound Zr(2)(WO(4))(PO(4))(2) |
title_full_unstemmed | First-Principles Structural, Mechanical, and Thermodynamic
Calculations of the Negative Thermal Expansion Compound Zr(2)(WO(4))(PO(4))(2) |
title_short | First-Principles Structural, Mechanical, and Thermodynamic
Calculations of the Negative Thermal Expansion Compound Zr(2)(WO(4))(PO(4))(2) |
title_sort | first-principles structural, mechanical, and thermodynamic
calculations of the negative thermal expansion compound zr(2)(wo(4))(po(4))(2) |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6644104/ https://www.ncbi.nlm.nih.gov/pubmed/31458228 http://dx.doi.org/10.1021/acsomega.8b02456 |
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