scholarly journals Correlation between creep-fatigue interaction and creep fracture mode for SUS 316 stainless steel subjected to combined creep-fatigue loading.

1984 ◽  
Vol 33 (375) ◽  
pp. 1533-1539 ◽  
Author(s):  
Koichi YAGI ◽  
Chiaki TANAKA ◽  
Kiyoshi KUBO
Keyword(s):  
Stainless Steel ◽  
Fracture Mode ◽  
Fatigue Loading ◽  
Creep Fracture ◽  
316 Stainless Steel ◽  
Creep Fatigue

scholarly journals Life prediction under creep-fatigue loading condition for SUS 316 stainless steel.

1986 ◽  
Vol 35 (389) ◽  
pp. 176-182 ◽  
Author(s):  
Koichi YAGI ◽  
Osamu KANEMARU ◽  
Kiyoshi KUBO ◽  
Chiaki TANAKA
Keyword(s):  
Stainless Steel ◽  
Life Prediction ◽  
Loading Condition ◽  
Fatigue Loading ◽  
316 Stainless Steel ◽  
Creep Fatigue

Crack Growth in Stainless Steel 304 under Creep-Fatigue Loading

2007 ◽  
Vol 353-358 ◽  
pp. 485-490 ◽  
Author(s):  
Y.M. Baik ◽  
K.S. Kim
Keyword(s):  
Stress Intensity Factor ◽  
Stainless Steel ◽  
Stress Intensity ◽  
Intensity Factor ◽  
Crack Growth ◽  
Growth Rates ◽  
Static Loading ◽  
Fatigue Loading ◽  
Creep Fatigue ◽  
Crack Growth Rates

Crack growth in compact specimens of type 304 stainless steel is studied at 538oC. Loading conditions include pure fatigue loading, static loading and fatigue loading with hold time. Crack growth rates are correlated with the stress intensity factor. A finite element analysis is performed to understand the crack tip field under creep-fatigue loading. It is found that fatigue loading interrupts stress relaxation around the crack tip and cause stress reinstatement, thereby accelerating crack growth compared with pure static loading. An effort is made to model crack growth rates under combined influence of creep and fatigue loading. The correlation with the stress intensity factor is found better when da/dt is used instead of da/dN. Both the linear summation rule and the dominant damage rule overestimate crack growth rates under creep-fatigue loading. A model is proposed to better correlate crack growth rates under creep-fatigue loading: 1 c f da da da dt dt dt Ψ −Ψ     =         , where Ψ is an exponent determined from damage under pure fatigue loading and pure creep loading. This model correlates crack growth rates for relatively small loads and low stress intensity factors. However, correlation becomes poor as the crack growth rate becomes large under a high level of load.

Creep fracture maps for 316 stainless steel

1979 ◽  
Vol 10 (11) ◽  
pp. 1635-1641 ◽  
Author(s):  
David A. Miller ◽  
Terence G. Langdon
Keyword(s):  
Stainless Steel ◽  
Creep Fracture ◽  
316 Stainless Steel

Evaluation of Creep-Fatigue Life Prediction Methods for Low-Carbon Nitrogen-Added 316 Stainless Steel

1998 ◽  
Vol 120 (2) ◽  
pp. 119-125 ◽  
Author(s):  
Yukio Takahashi
Keyword(s):  
Stainless Steel ◽  
Fatigue Life ◽  
Life Prediction ◽  
Fatigue Life Prediction ◽  
Prediction Methods ◽  
Secondary Creep ◽  
Low Carbon ◽  
316 Stainless Steel ◽  
Creep Fatigue ◽  
Exhaustion Method

Low-carbon, medium-nitrogen 316 stainless steel is a principal candidate for a main structural material of a demonstration fast breeder reactor plant in Japan. A number of long-term creep tests and creep-fatigue tests have been conducting for two heats of the steel. Two representative creep-fatigue life prediction methods, i.e., time fraction rule and ductility exhaustion method were applied. An introduction of a simple viscous strain term improved the description of stress relaxation behavior and only the conventional (primary plus secondary) creep strain was assumed to contribute to creep damage in the ductility exhaustion method. The present ductility exhaustion approach was found to have very good accuracy in creep-fatigue life prediction, while the time fraction rule overpredicted failure life as large as a factor of 30.

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