Development of a grain growth model for U3Si2 using experimental data, phase field simulation and molecular dynamics

The purpose of this work is to develop a model for normal grain growth in U3Si2. The average grain boundary energy was determined from previously published molecular dynamics simulations. The grain growth kinetics were quantified at various temperatures by annealing nanocrystalline samples. The mobi...

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Published in:Journal of nuclear materials Vol. 532; no. C; p. 152069
Main Authors: Cheniour, Amani, Tonks, Michael R., Gong, Bowen, Yao, Tiankai, He, Lingfeng, Harp, Jason M., Beeler, Benjamin, Zhang, Yongfeng, Lian, Jie
Format: Journal Article
Language:English
Published: Amsterdam Elsevier B.V 15-04-2020
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Abstract The purpose of this work is to develop a model for normal grain growth in U3Si2. The average grain boundary energy was determined from previously published molecular dynamics simulations. The grain growth kinetics were quantified at various temperatures by annealing nanocrystalline samples. The mobility was determined by comparing phase field grain growth simulations to the experimental data. From these various methods, we found that the average grain size D in U3Si2 can be estimated over time t using the equation D2−D02=2αMγt, where D0 is the initial average grain size, the geometry factor α=0.96, the average grain boundary mobility M=6.30×10−18e−0.33[eV]kbTm4/(Js) with the Boltzmann constant kb and temperature T, and the average grain boundary energy has been found as a function of temperature, e.g. γ¯=0.83 J/m2 at 673 K. •The grain growth constant and activation energy were obtained from isothermal annealing experiments on U3Si2 lamellae.•The grain growth geometric constant was calculated using several 3D phase field grain growth simulations.•The grain boundary mobility was determined from experimental data, grain boundary energy, and phase field simulations.•More grain growth occurs in U3Si2 than in UO2 at 1200 K.•Grain growth is more rapid in UO2 than in U3Si2 at their respective centerline temperatures.
AbstractList The purpose of this work is to develop a model for normal grain growth in U3Si2. The average grain boundary energy was determined from previously published molecular dynamics simulations. The grain growth kinetics were quantified at various temperatures by annealing nanocrystalline samples. The mobility was determined by comparing phase field grain growth simulations to the experimental data. From these various methods, we found that the average grain size D in U3Si2 can be estimated over time t using the equation D2−D02=2αMγt, where D0 is the initial average grain size, the geometry factor α=0.96, the average grain boundary mobility M=6.30×10−18e−0.33[eV]/kbT m4/(Js) with the Boltzmann constant kb and temperature T, and the average grain boundary energy has been found as a function of temperature, e.g. γ¯=0.83 J/m2 at 673 K.
The purpose of this work is to develop a model for normal grain growth in U3Si2. The average grain boundary energy was determined from previously published molecular dynamics simulations. The grain growth kinetics were quantified at various temperatures by annealing nanocrystalline samples. The mobility was determined by comparing phase field grain growth simulations to the experimental data. From these various methods, we found that the average grain size D in U3Si2 can be estimated over time t using the equation D2−D02=2αMγt, where D0 is the initial average grain size, the geometry factor α=0.96, the average grain boundary mobility M=6.30×10−18e−0.33[eV]kbTm4/(Js) with the Boltzmann constant kb and temperature T, and the average grain boundary energy has been found as a function of temperature, e.g. γ¯=0.83 J/m2 at 673 K. •The grain growth constant and activation energy were obtained from isothermal annealing experiments on U3Si2 lamellae.•The grain growth geometric constant was calculated using several 3D phase field grain growth simulations.•The grain boundary mobility was determined from experimental data, grain boundary energy, and phase field simulations.•More grain growth occurs in U3Si2 than in UO2 at 1200 K.•Grain growth is more rapid in UO2 than in U3Si2 at their respective centerline temperatures.
ArticleNumber 152069
Author Beeler, Benjamin
Lian, Jie
Zhang, Yongfeng
Gong, Bowen
Cheniour, Amani
Tonks, Michael R.
He, Lingfeng
Yao, Tiankai
Harp, Jason M.
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  givenname: Michael R.
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  fullname: Yao, Tiankai
  organization: Idaho National Laboratory, Idaho Falls, ID, 83402, USA
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  organization: Idaho National Laboratory, Idaho Falls, ID, 83402, USA
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  organization: Department of Mechanical, Aerospace and Nuclear Engineering, Rensselaer Polytechnic Institute, Troy, NY, 12180, USA
BackLink https://www.osti.gov/biblio/1602301$$D View this record in Osti.gov
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Keywords U3Si2
Grain boundary mobility
Isothermal annealing experiments
Grain growth
Phase field
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Snippet The purpose of this work is to develop a model for normal grain growth in U3Si2. The average grain boundary energy was determined from previously published...
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SubjectTerms Computer simulation
Experimental data
Grain boundaries
Grain boundary mobility
Grain growth
Grain size
Growth kinetics
Growth models
Isothermal annealing experiments
Mobility
Molecular dynamics
Particle size
Phase field
Temperature
U3Si2
Uranium silicide
Title Development of a grain growth model for U3Si2 using experimental data, phase field simulation and molecular dynamics
URI https://dx.doi.org/10.1016/j.jnucmat.2020.152069
https://www.proquest.com/docview/2437944142
https://www.osti.gov/biblio/1602301
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