论文

利用纳米压入的反演分析法确定金属材料的塑性性能

  • 马永 ,
  • 姚晓红 ,
  • 张翔宇 ,
  • 田林海 ,
  • 树学峰 ,
  • 唐宾
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  • 1.太原理工大学表面工程研究所, 太原 030024
    2.太原理工大学应用力学与生物医药工程研究所, 太原 030024
马永, 男, 1980年生, 博士生

收稿日期: 2010-11-03

  修回日期: 2010-12-10

  网络出版日期: 2011-03-11

基金资助

国家高技术研究发展计划项目2007AA03Z521, 国家自然科学基金项目50771070和山西省科技攻关项目20100321078-02资助

EXTRACT THE PLASTIC PROPERTIES OF METALS USING REVERSE ANALYSIS OF NANOINDENTATION TEST

  • MA Yong ,
  • YAO Xiao-Hong ,
  • ZHANG Xiang-Yu ,
  • TIAN Lin-Hai ,
  • SUN Hua-Feng ,
  • TANG Bin
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  • 1. Institute of Surface Engineering, Taiyuan University of Technology, Taiyuan 030024
    2. Institute of Applied Mechanics and Biomedical Engineering, Taiyuan University of Technology, Taiyuan 030024

Received date: 2010-11-03

  Revised date: 2010-12-10

  Online published: 2011-03-11

Supported by

Supported by High Technology Research and Development Program of China (No.2007AA03Z521), National Natural Science Foundation of China (No.50771070) and Shanxi Province Science and Technology Key Project (No.20100321078–02)

摘要

建立了一种确定金属材料塑性性能的方法, 即利用有限元数值模拟对纳米压入过程进行反演分析, 确定金属材料的屈服极限和应变强化指数.首先在不考虑材料加工硬化的情况下, 对纳米压入过程进行反演修正模拟,当模拟曲线同正向分析曲线相吻合时, 确定金属材料的代表性应力;其次在考虑不同应变强化指数的情况下, 采用相同的方法确定金属材料的代表性应变; 最后结合量纲分析确定金属材料的应变强化指数,继而确定金属材料的屈服极限. 经过实验验证, 该方法具有较高的精度.

本文引用格式

马永 , 姚晓红 , 张翔宇 , 田林海 , 树学峰 , 唐宾 . 利用纳米压入的反演分析法确定金属材料的塑性性能[J]. 金属学报, 2011 , 47(3) : 321 -326 . DOI: 10.3724/SP.J.1037.2010.00583

Abstract

Using traditional methods to evaluate mechanical properties of bulk materials is not applicable for metal surface studying and metals with very small volume. Nanoindentation testing at very low load is a new successful technique for study of mechanical properties on small scales or near surfaces. However, so far there is not a robust approach to determine plastic properties of metal materials using nanoindentation test. The aim of this paper is to present a method for determining the plastic properties, e.g. the true plastic stress–true plastic strain relation of metals combining nanonindentation test and finite element simulation. This methodology contains three main parts. Firstly, considering the special case of metals without strain hardening, the representative stress εr is determined by varying assumed representative stress over a wide range until the reverse and forward loading curves are consistent. Then, also by comparing the reverse and forward loading curves, the representative strain "r is obtained, but with different values of strain hardening exponent n, which are in the range of 0—0.6. Secondly, a series of simulations are performed for 124 combinations of each parameter (Eσy, nν) expressing the elastic–plastic behaviors of the universal engineering metals. Fom the computational results, a dimensinless function ∏u is constructed, and then the strain hardening exponent idetermined. At last, substituting the strain hardening exponent n into the power law constitution, the yield stress σy of metals is acquired. The examination of 5 kinds of metals from the forward analysis metal materials indicates that the dimensionless function ∏u has generality and the strain hardening exponent has stability and uniqueness. The accuracy of this method is also examined by comparing the elasto–plastic properties of practical metal AISI 304 steel obtained from nanoindentation test and finite element simulation with the tensile test results. In order to make the reverse analysis results get higher precision, in the practical applcation of this technique, the test error of nanoindentation should be maximally reduced.

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