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A comprehensive method to identify the kinetics of static recrystallization using the hot torsion test results with an inverse solution.

Authors :
S Khoddam
P D Hodgson
Source :
Modelling & Simulation in Materials Science & Engineering. Dec2014, Vol. 22 Issue 8, p1-1. 1p.
Publication Year :
2014

Abstract

Many difficulties exist in directly following the static recrystallization of metals, particularly during hot working. Indirect measurement of static recrystallization has been extensively performed in the literature where, for example, the recrystallization behavior of austenite in steels has commonly been measured indirectly using the fractional softening method. This method relies on the yield stress changes during recrystallization which are physically simulated by hot torsion or compression tests. However, the inherent heterogeneity of deformation during a mechanical test leads to a non-uniform static recrystallization distribution in the test sample. This, in turn, poses a serious question concerning the reliability of the measurement since the stress calculation techniques during recrystallization are not adequately developed in the existing literature.This paper develops a computer-based method to account for heterogeneous deformation during fractional softening measurements based on the hot torsion test data. The importance of the fractional softening gradient in determining the kinetics is emphasized and deficiencies in our understanding of the basic mechanisms are highlighted. A computer-based method is introduced to generate the experimental and computational components in a cost function. The cost function is then utilized by an inverse solution to calibrate the design parameters in a static recrystallization model.A [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
09650393
Volume :
22
Issue :
8
Database :
Academic Search Index
Journal :
Modelling & Simulation in Materials Science & Engineering
Publication Type :
Academic Journal
Accession number :
99386412
Full Text :
https://doi.org/10.1088/0965-0393/22/8/085010