Evaluation of Reaction Rate Theory and Monte Carlo Methods for Application to Radiation-Induced Microstructural Characterization

Stoller, Roger E¹  Golubov, Stanislav I¹  Becquart, C. S.²  Domain, C.³ 

[1]ORNL

[2]Universite de Lille

[3]EDF R&D, Clamart, France

关键词: APPROXIMATIONS;    COMPUTERS;    CREEP;    DEFECTS;    DIFFUSION;    DISLOCATIONS;    EVALUATION;    IRRADIATION;    KINETICS;    MICROSTRUCTURE;    MONTE CARLO METHOD;    NUCLEATION;    POINT DEFECTS;    RADIATIONS;   

DOI  :  10.2172/969944
RP-ID  :  ORNL/TM-2007/137
PID  :  OSTI ID: 969944
Others  :  Other: AT6020100
Others  :  AF3625200
Others  :  ERAT725
Others  :  NEAF265
Others  :  TRN: US201002%%1025

学科分类：社会科学、人文和艺术（综合）

美国|英语

来源: SciTech Connect

【 摘 要 】

The multiscale modeling scheme encompasses models from the atomistic to the continuum scale. Phenomena at the mesoscale are typically simulated using reaction rate theory, Monte Carlo, or phase field models. These mesoscale models are appropriate for application to problems that involve intermediate length scales, and timescales from those characteristic of diffusion to long-term microstructural evolution (~s to years). Although the rate theory and Monte Carlo models can be used simulate the same phenomena, some of the details are handled quite differently in the two approaches. Models employing the rate theory have been extensively used to describe radiation-induced phenomena such as void swelling and irradiation creep. The primary approximations in such models are time- and spatial averaging of the radiation damage source term, and spatial averaging of the microstructure into an effective medium. Kinetic Monte Carlo models can account for these spatial and temporal correlations; their primary limitation is the computational burden which is related to the size of the simulation cell. A direct comparison of RT and object kinetic MC simulations has been made in the domain of point defect cluster dynamics modeling, which is relevant to the evolution (both nucleation and growth) of radiation-induced defect structures. The primary limitations of the OKMC model are related to computational issues. Even with modern computers, the maximum simulation cell size and the maximum dose (typically much less than 1 dpa) that can be simulated are limited. In contrast, even very detailed RT models can simulate microstructural evolution for doses up 100 dpa or greater in clock times that are relatively short. Within the context of the effective medium, essentially any defect density can be simulated. Overall, the agreement between the two methods is best for irradiation conditions which produce a high density of defects (lower temperature and higher displacement rate), and for materials that have a relatively high density of fixed sinks such as dislocations.