Cyclic hardening and softening of high-strength steels

316L and P91 steels, commonly used for high-temperature applications in power plants, experience low-cycle fatigue. In this work, the cyclic stress-strain behaviour of 316L and P91 materials was analyzed. Experimental data from the material's hysteresis loops and cyclic stress response were used to derive material parameters for numerical simulation of the cyclic behaviour. The displacement-controlled model with strain amplitudes of 0.4% and 0.6% and a constant strain rate of 0.001 s-1 was used in the simulation. The simulation results show that 316L stainless steel exhibits cyclic hardening, with the maximum stress increasing from 311.3 MPa in the first cycle to 354.7 MPa at the half-cycle, corresponding to approximately 14% cyclic hardening. In contrast, P91 steel exhibits cyclic softening of about 8.3%, as the stress decreases from 497.9 MPa in the first cycle to 456.7 MPa at the half cycle. The findings also demonstrated that tension and compression loadings with larger strain amplitudes produced higher maximum stress. It also demonstrates that higher strain amplitudes result in a greater decrease in stress near the half cycle because hardening/softening is more pronounced at higher strain amplitudes.

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Publication Details

Journal
JOURNAL OF MECHANICAL ENGINEERING AND SCIENCES
Published
2026-03-31
DOI
https://doi.org/10.15282/jmes.20.1.2026.3.0863
Primary Topic
High Temperature Alloys and Creep
Type
article
Field-Weighted Citation Impact
0.00

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article

Cyclic hardening and softening of high-strength steels

N. A. Rahmat, Nasrul Azuan Alang, Norhaida Ab Razak
JOURNAL OF MECHANICAL ENGINEERING AND SCIENCES
High Temperature Alloys and Creep
article

Cyclic hardening and softening of high-strength steels

N. A. Rahmat, Nasrul Azuan Alang, Norhaida Ab Razak
article en

Abstract

316L and P91 steels, commonly used for high-temperature applications in power plants, experience low-cycle fatigue. In this work, the cyclic stress-strain behaviour of 316L and P91 materials was analyzed. Experimental data from the material's hysteresis loops and cyclic stress response were used to derive material parameters for numerical simulation of the cyclic behaviour. The displacement-controlled model with strain amplitudes of 0.4% and 0.6% and a constant strain rate of 0.001 s-1 was used in the simulation. The simulation results show that 316L stainless steel exhibits cyclic hardening, with the maximum stress increasing from 311.3 MPa in the first cycle to 354.7 MPa at the half-cycle, corresponding to approximately 14% cyclic hardening. In contrast, P91 steel exhibits cyclic softening of about 8.3%, as the stress decreases from 497.9 MPa in the first cycle to 456.7 MPa at the half cycle. The findings also demonstrated that tension and compression loadings with larger strain amplitudes produced higher maximum stress. It also demonstrates that higher strain amplitudes result in a greater decrease in stress near the half cycle because hardening/softening is more pronounced at higher strain amplitudes.

JOURNAL OF MECHANICAL ENGINEERING AND SCIENCES
Universiti Malaysia Pahang Al-Sultan Abdullah (MY)
Universiti Malaysia Pahang
Openalex Percentile: Top 37%
High Temperature Alloys and Creep
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