Predicting the critical stress for initiation of dynamic recrystallization

被引:224
|
作者
Najafizadeh, Abbas [1 ]
Jonas, John J.
机构
[1] Isfahan Univ Technol, Dept Mat Engn, Esfahan, Iran
[2] McGill Univ, Dept Met Engn, Montreal, PQ H3A 2B2, Canada
关键词
dynamic recrystallization; critical stress; strain hardening rate; 304 H stainless steel; modeling;
D O I
10.2355/isijinternational.46.1679
中图分类号
TF [冶金工业];
学科分类号
0806 ;
摘要
The critical stress for initiation of dynamic recrystallization (DRX) can be identified from the inflection point on the strain hardening rate (theta=d sigma/d epsilon) versus flow stress (a) curve. This kind of curve can be described by an equation that fits the experimental theta-sigma data from zero to the peak stress. Such a curve must have an inflection point and the simplest relation that has such properties is a third order equation. Hot compression tests were carried out on a 304 H stainless steel over the temperature range 900-1 100 degrees C and strain rate range 0.01-1s(-1) to a strain of 1. An appropriate third order equation was fitted to the strain hardening data. The results show that the critical stress at initiation sigma(c)=-B/3A where A and B are coefficients of the third order equation. It is evident that this value depends on the deformation conditions. The stress-strain curve was then normalized with respect to the peak stress, leading to a normalized value of the critical stress (u(c)) equal to u(c)=sigma(c)/sigma(p)=-B'/3A'. Here A' and B' are coefficients of the normalized third order equation. This value is constant and independent of the deformation conditions.
引用
收藏
页码:1679 / 1684
页数:6
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