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关于从锥形压痕识别幂律蠕变参数

On the identification of power-law creep parameters from conical indentation.

作者信息

Zhang Yupeng, Needleman Alan

机构信息

Department of Materials Science and Engineering, Texas A&M University, College Station, TX, USA.

出版信息

Proc Math Phys Eng Sci. 2021 Aug;477(2252):20210233. doi: 10.1098/rspa.2021.0233. Epub 2021 Aug 18.

DOI:10.1098/rspa.2021.0233
PMID:35153575
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8371371/
Abstract

Load and hold conical indentation responses calculated for materials having creep stress exponents of 1.15, 3.59 and 6.60 are regarded as input 'experimental' responses. A Bayesian-type statistical approach (Zhang 2019 , 011002 (doi:10.1115/1.4041352)) is used to infer power-law creep parameters, the creep exponent and the associated pre-exponential factor, from noise-free as well as noise-contaminated indentation data. A database for the Bayesian-type analysis is created using finite-element calculations for a coarse set of parameter values with interpolation used to create the refined database used for parameter identification. Uniaxial creep and stress relaxation responses using the identified creep parameters provide a very good approximation to those of the 'experimental' materials with stress exponents of 1.15 and 3.59. The sensitivity to noise increases with increasing stress exponent. The uniaxial creep response is more sensitive to the accuracy of the predictions than the uniaxial stress relaxation response. Good agreement with the indentation response does not guarantee good agreement with the uniaxial response. If the noise level is sufficiently small, the model of Bower (1993 , 97-124 ()) provides a good fit to the 'experimental' data for all values of creep stress exponent considered, while the model of Ginder (2018 , 552-562 ()) provides a good fit for a creep stress exponent of 1.15.

摘要

针对蠕变应力指数分别为1.15、3.59和6.60的材料计算得到的加载并保持锥形压痕响应被视为输入的“实验”响应。采用贝叶斯型统计方法(Zhang 2019,011002(doi:10.1115/1.4041352))从无噪声以及受噪声污染的压痕数据中推断幂律蠕变参数、蠕变指数和相关的预指数因子。使用有限元计算为一组粗略的参数值创建贝叶斯型分析数据库,并通过插值创建用于参数识别的精细数据库。使用识别出的蠕变参数得到的单轴蠕变和应力松弛响应与蠕变应力指数为1.15和3.59的“实验”材料的响应非常接近。随着应力指数的增加,对噪声的敏感度也增加。单轴蠕变响应比单轴应力松弛响应对预测精度更敏感。与压痕响应良好吻合并不保证与单轴响应也良好吻合。如果噪声水平足够小,对于所考虑的所有蠕变应力指数值,Bower(1993,97 - 124())的模型能很好地拟合“实验”数据,而Ginder(2018,552 - 562())的模型对于蠕变应力指数为1.15时能很好地拟合。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/c331/8371371/1595adf9c368/rspa20210233f08.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/c331/8371371/67253a30448a/rspa20210233f01.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/c331/8371371/0f26ab64083b/rspa20210233f02.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/c331/8371371/b9e27023f523/rspa20210233f03.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/c331/8371371/1595adf9c368/rspa20210233f08.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/c331/8371371/67253a30448a/rspa20210233f01.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/c331/8371371/0f26ab64083b/rspa20210233f02.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/c331/8371371/b9e27023f523/rspa20210233f03.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/c331/8371371/1595adf9c368/rspa20210233f08.jpg

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