Tellurium Oxides: Thermodynamics and Phase Relations in the Te–O System

IF 1.7 4区 材料科学 Q4 CHEMISTRY, PHYSICAL Journal of Phase Equilibria and Diffusion Pub Date : 2025-02-13 DOI:10.1007/s11669-025-01175-6
S. Gossé
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引用次数: 0

Abstract

The Te–O phase diagram and the TeO2 thermodynamic properties are of interest for many industrial fields: nuclear applications, steel making industry and chalcogenide glass processes. Both, the thermodynamic properties and phase diagram of this relevant binary system were reviewed and assessed using the Calphad method. From this assessment, the standard Gibbs free energy and corresponding heat capacity of the binary oxides are calculated as:

$$\begin{gathered} \Delta_{{\text{f}}} {\text{G}}_{{{\text{TeO}}_{2} }}^{ \circ } \left( {{\text{KJ}} \cdot {\text{mol}}^{ - 1} } \right) = - 109.646 + 0.1034 \cdot T - 0.0064 \cdot T \cdot \ln (T) \hfill \\ {\text{C}}_{{{\text{p}}_{{{\text{TeO}}_{2} }} }} \left( {{\text{J}} \cdot {\text{K}} \cdot {\text{mol}}^{ - 1} } \right) = 19.59 + 0.0101 \cdot {\text{T}} - 1.6 \cdot 10 ^{- 6}.T^{2} - 186517 \cdot T^{ - 2} \hfill \\ \end{gathered}$$
$$\begin{gathered} \Delta_{{\text{f}}} {\text{G}}_{{{\text{Te}}_{2} {\text{O}}_{5} }}^{ \circ } \left( {{\text{KJ}} \cdot {\text{mol}}^{ - 1} } \right) = - 104.81 + 0.1175 \cdot T - 0.0077 \cdot T \cdot \ln (T) \hfill \\ {\text{C}}_{{{\text{p}}_{{{\text{Te}}_{2} {\text{O}}_{5} }} }} \left( {{\text{J}} \cdot {\text{K}}^{ - 1} \cdot {\text{mol}}^{ - 1} } \right) = 19.86 + 0.0091 \cdot T - 285181 \cdot T^{ - 2} \hfill \\ \end{gathered}$$
$$\begin{gathered} \Delta_{{\text{f}}} {\text{G}}_{{{\text{TeO}}_{3} }}^{ \circ } \left( {{\text{KJ}} \cdot {\text{mol}}^{ - 1} } \right) = - 92.79 + 0.111 \cdot T - 0.00776 \cdot T \cdot \ln (T) \hfill \\ {\text{C}}_{{{\text{PTeO}}_{3} }} \left( {{\text{J}} \cdot {\text{K}}^{ - 1} \cdot {\text{mol}}^{ - 1} } \right) = 17.475 + 0.013 \cdot {\text{T}} - 2.085 \cdot 10^{ - 6} \cdot T^{2} - 280000 \cdot T^{ - 2} \hfill \\ \end{gathered}$$
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碲氧化物:Te-O体系的热力学和相关系
Te-O相图和TeO2热力学性质对许多工业领域都很感兴趣:核应用,炼钢工业和硫系玻璃工艺。用calphhad方法对该二元体系的热力学性质和相图进行了评述和评价。由此计算出二元氧化物的标准吉布斯自由能和相应的热容为:$$\begin{gathered} \Delta_{{\text{f}}} {\text{G}}_{{{\text{TeO}}_{2} }}^{ \circ } \left( {{\text{KJ}} \cdot {\text{mol}}^{ - 1} } \right) = - 109.646 + 0.1034 \cdot T - 0.0064 \cdot T \cdot \ln (T) \hfill \\ {\text{C}}_{{{\text{p}}_{{{\text{TeO}}_{2} }} }} \left( {{\text{J}} \cdot {\text{K}} \cdot {\text{mol}}^{ - 1} } \right) = 19.59 + 0.0101 \cdot {\text{T}} - 1.6 \cdot 10 ^{- 6}.T^{2} - 186517 \cdot T^{ - 2} \hfill \\ \end{gathered}$$$$\begin{gathered} \Delta_{{\text{f}}} {\text{G}}_{{{\text{Te}}_{2} {\text{O}}_{5} }}^{ \circ } \left( {{\text{KJ}} \cdot {\text{mol}}^{ - 1} } \right) = - 104.81 + 0.1175 \cdot T - 0.0077 \cdot T \cdot \ln (T) \hfill \\ {\text{C}}_{{{\text{p}}_{{{\text{Te}}_{2} {\text{O}}_{5} }} }} \left( {{\text{J}} \cdot {\text{K}}^{ - 1} \cdot {\text{mol}}^{ - 1} } \right) = 19.86 + 0.0091 \cdot T - 285181 \cdot T^{ - 2} \hfill \\ \end{gathered}$$$$\begin{gathered} \Delta_{{\text{f}}} {\text{G}}_{{{\text{TeO}}_{3} }}^{ \circ } \left( {{\text{KJ}} \cdot {\text{mol}}^{ - 1} } \right) = - 92.79 + 0.111 \cdot T - 0.00776 \cdot T \cdot \ln (T) \hfill \\ {\text{C}}_{{{\text{PTeO}}_{3} }} \left( {{\text{J}} \cdot {\text{K}}^{ - 1} \cdot {\text{mol}}^{ - 1} } \right) = 17.475 + 0.013 \cdot {\text{T}} - 2.085 \cdot 10^{ - 6} \cdot T^{2} - 280000 \cdot T^{ - 2} \hfill \\ \end{gathered}$$
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来源期刊
Journal of Phase Equilibria and Diffusion
Journal of Phase Equilibria and Diffusion 工程技术-材料科学:综合
CiteScore
2.50
自引率
7.10%
发文量
70
审稿时长
1 months
期刊介绍: The most trusted journal for phase equilibria and thermodynamic research, ASM International''s Journal of Phase Equilibria and Diffusion features critical phase diagram evaluations on scientifically and industrially important alloy systems, authored by international experts. The Journal of Phase Equilibria and Diffusion is critically reviewed and contains basic and applied research results, a survey of current literature and other pertinent articles. The journal covers the significance of diagrams as well as new research techniques, equipment, data evaluation, nomenclature, presentation and other aspects of phase diagram preparation and use. Content includes information on phenomena such as kinetic control of equilibrium, coherency effects, impurity effects, and thermodynamic and crystallographic characteristics. The journal updates systems previously published in the Bulletin of Alloy Phase Diagrams as new data are discovered.
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