TY - JOUR
T1 - An advanced mean field dislocation density reliant physical model to predict the creep deformation of 304HCu austenitic stainless steel
AU - Mehrotra, Pankhuri
AU - Kumar, Nilesh
AU - George, Alphy
AU - Sahoo, Kanhu Charan
AU - Ganesan, Vaidyanathan
AU - Ahmadi, Mohammad Reza
AU - Trivedi, Shivam
AU - Yadav, Surya D.
N1 - Funding Information:
The research work was carried out in the framework of projects DST/INSPIRE/04/2018/003390 and DST/INT/BMWF/Austria/P-11/2020 (Development of mesoscale models to describe hot deformation and creep of low SFE materials). Authors would like to thank OEAD Austria and DST India for the financial support. Authors would like to thank Prof. Cecilia Poletti (TU Graz) for the valuable discussions on various aspects of physical based modelling.
Funding Information:
The research work was carried out in the framework of projects DST/INSPIRE/04/2018/003390 and DST/INT/BMWF/Austria/P-11/2020 (Development of mesoscale models to describe hot deformation and creep of low SFE materials). Authors would like to thank OEAD Austria and DST India for the financial support. Authors would like to thank Prof. Cecilia Poletti (TU Graz) for the valuable discussions on various aspects of physical based modelling.
Publisher Copyright:
© 2022 Elsevier Ltd
PY - 2022/8
Y1 - 2022/8
N2 - Physical based creep modelling enables to understand the life-limiting factors that are required for a safe and economic operation of power plant components. Thus, herein an improved physical approach to address the creep behavior of 304HCu austenitic stainless steel is presented. This approach combines a dislocation density reliant physical model with a continuum damage mechanics (CDM) model. Two different dislocation densities: mobile and forest, and dislocation mean free path are used to describe the substructure in order to model the creep strain. The original Orowan's equation for estimating creep strain rate is modified employing CDM based softening parameters to take account of damage causing tertiary creep. The model is advantageous in the sense that with the ongoing creep, the evolution of different variables that are dislocation densities, dislocation mobility, dislocation velocity, internal stress, effective stress and damage evolution is tracked and discussed thoroughly. Furthermore, the model output is corroborated with experimental creep data of 304HCu steel. The predicted values of forest dislocation density, mobile dislocation density, mean free path, internal stress, effective stress, dislocation mobility and dislocation velocity are in the range of 7.91 × 1011 – 1.01 × 1013 m−2, 8.16 × 1010 – 4.56 × 1011 m−2, 9.35 – 9.80 µm, 11.70 – 35.50 MPa, 86.0 – 165.0 MPa, 1.68 × 10−9 – 2.11 × 10−7 Pa−1s−1 and 6.48 × 10−11 – 7.45 × 10−9 m/s, respectively, at the end of simulation.
AB - Physical based creep modelling enables to understand the life-limiting factors that are required for a safe and economic operation of power plant components. Thus, herein an improved physical approach to address the creep behavior of 304HCu austenitic stainless steel is presented. This approach combines a dislocation density reliant physical model with a continuum damage mechanics (CDM) model. Two different dislocation densities: mobile and forest, and dislocation mean free path are used to describe the substructure in order to model the creep strain. The original Orowan's equation for estimating creep strain rate is modified employing CDM based softening parameters to take account of damage causing tertiary creep. The model is advantageous in the sense that with the ongoing creep, the evolution of different variables that are dislocation densities, dislocation mobility, dislocation velocity, internal stress, effective stress and damage evolution is tracked and discussed thoroughly. Furthermore, the model output is corroborated with experimental creep data of 304HCu steel. The predicted values of forest dislocation density, mobile dislocation density, mean free path, internal stress, effective stress, dislocation mobility and dislocation velocity are in the range of 7.91 × 1011 – 1.01 × 1013 m−2, 8.16 × 1010 – 4.56 × 1011 m−2, 9.35 – 9.80 µm, 11.70 – 35.50 MPa, 86.0 – 165.0 MPa, 1.68 × 10−9 – 2.11 × 10−7 Pa−1s−1 and 6.48 × 10−11 – 7.45 × 10−9 m/s, respectively, at the end of simulation.
KW - Creep damage
KW - Creep modelling
KW - Dislocation density
KW - Dislocation mobility
KW - Internal stress
UR - http://www.scopus.com/inward/record.url?scp=85135920042&partnerID=8YFLogxK
U2 - 10.1016/j.mtcomm.2022.104128
DO - 10.1016/j.mtcomm.2022.104128
M3 - Article
AN - SCOPUS:85135920042
SN - 2352-4928
VL - 32
JO - Materials Today Communications
JF - Materials Today Communications
M1 - 104128
ER -