Influence of cerium on the creep properties of the austenitic stainless steel 253MA

1988 ◽  
Vol 6 (3) ◽  
pp. 153-157 ◽  
Author(s):  
Y. Maode ◽  
R. Sandström
2013 ◽  
Vol 83 ◽  
pp. 49-57 ◽  
Author(s):  
Kyu-Ho Lee ◽  
Jin-Yoo Suh ◽  
Joo-Youl Huh ◽  
Dae-Bum Park ◽  
Sung-Min Hong ◽  
...  

Materials ◽  
2020 ◽  
Vol 13 (6) ◽  
pp. 1297 ◽  
Author(s):  
Grzegorz Golański ◽  
Adam Zieliński ◽  
Marek Sroka ◽  
Jacek Słania

The physical metallurgical tests were performed on the test samples made of HR3C steel, taken from a section of a pipeline in the as-received condition and after approximately 26,000 h of service at 550 °C. In the as-received condition, the test material had austenitic microstructure with numerous large primary Z-phase precipitates inside the grains. The service of the test steel mainly contributed to the precipitation processes inside the grains and at the grain boundaries. After service, the following precipitates were identified in the microstructure of the test steel: Z-phase (NbCrN) and M23C6 carbides. The Z-phase precipitates were observed inside the grains, whereas M23C6 carbides - at the boundaries where they formed the so-called continuous grid. The service of the test steel contributed to the growth of the strength properties, determined both at room and elevated temperature (550, 600 °C), compared to the as-received condition. Moreover, the creep properties of HR3C steel after service were higher than those of the material in the as-received condition. The increase in the strength properties and creep resistance was connected with the growth of strengthening of the test steel by the precipitation of Z-phase and M23C6 carbides.


2013 ◽  
Vol 438 (1-3) ◽  
pp. 51-57 ◽  
Author(s):  
V.D. Vijayanand ◽  
P. Parameswaran ◽  
M. Nandagopal ◽  
S. Panneer Selvi ◽  
K. Laha ◽  
...  

Author(s):  
R. Gonzalez ◽  
L. Bru

The analysis of stacking fault tetrahedra (SFT) in fatigued metals (1,2) is somewhat complicated, due partly to their relatively low density, but principally to the presence of a very high density of dislocations which hides them. In order to overcome this second difficulty, we have used in this work an austenitic stainless steel that deforms in a planar mode and, as expected, examination of the substructure revealed planar arrays of dislocation dipoles rather than the cellular structures which appear both in single and polycrystals of cyclically deformed copper and silver. This more uniform distribution of dislocations allows a better identification of the SFT.The samples were fatigue deformed at the constant total strain amplitude Δε = 0.025 for 5 cycles at three temperatures: 85, 293 and 773 K. One of the samples was tensile strained with a total deformation of 3.5%.


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