Título

CREEP BEHAVIOUR OF TYPE 310 STAINLESS STEEL. PART 2: ANALYSIS BASED ON THE STUDY OF TRANSIENTS AFTER STRESS REDUCTION EXPERIMENTS

CREEP BEHAVIOUR OF TYPE 310 STAINLESS STEEL. PART 2: ANALYSIS BASED ON THE STUDY OF TRANSIENTS AFTER STRESS REDUCTION EXPERIMENTS

Autoria

Junior, Archimedes Contin; Bueno, Levi de Oliveira

DOI

10.5151/2594-5327-23661

Downloads

Baixar Artigo 96 Downloads

Resumo

Stress-drop experiments during secondary creep in AISI 310 stainless steel were performed at seven stress levels in the range from 70 to 210MPa, at 700oC. Incubation periods were systematically detected following the stress reductions and their duration measured. Recovery kinetics parameters and friction stress (o) data were determined by extrapolation using a physical equation suggested in literature for the process. The friction stress was found to increase linearly with applied stress in the range from 70 to 120MPa and to reach a constant value o ≈ 66 MPa from 120 to 210 MPa. The initial friction stress level of the material was also estimated to be about 6 MPa. Secondary creep rates could be expressed by a single power law relation with n ≈ 3.5 in terms of the effective stress (o). Initial creep rates could also be expressed by the same power law relation in the range from 40 to 140 MPa. Assumptions are put forward for the variation of the friction stress in secondary creep stage, in the interval from 250 to 375 MPa, so that secondary creep rate in the whole interval from 70 to 375 MPa can be expressed by: έs=4.943x10-14.(–o)3.85. Normalization of the effective stress by the yield stress0.05 of the material at 700oC, gives the relation: έs=5.86x10-6.[(–o)/0.05]3.85. This expression is not fully consistent with the universal equation proposed by Evans and Harrison for secondary creep in metallic materials.

 

Stress-drop experiments during secondary creep in AISI 310 stainless steel were performed at seven stress levels in the range from 70 to 210MPa, at 700oC. Incubation periods were systematically detected following the stress reductions and their duration measured. Recovery kinetics parameters and friction stress (o) data were determined by extrapolation using a physical equation suggested in literature for the process. The friction stress was found to increase linearly with applied stress in the range from 70 to 120MPa and to reach a constant value o ≈ 66 MPa from 120 to 210 MPa. The initial friction stress level of the material was also estimated to be about 6 MPa. Secondary creep rates could be expressed by a single power law relation with n ≈ 3.5 in terms of the effective stress (o). Initial creep rates could also be expressed by the same power law relation in the range from 40 to 140 MPa. Assumptions are put forward for the variation of the friction stress in secondary creep stage, in the interval from 250 to 375 MPa, so that secondary creep rate in the whole interval from 70 to 375 MPa can be expressed by: έs=4.943x10-14.(–o)3.85. Normalization of the effective stress by the yield stress0.05 of the material at 700oC, gives the relation: έs=5.86x10-6.[(–o)/0.05]3.85. This expression is not fully consistent with the universal equation proposed by Evans and Harrison for secondary creep in metallic materials.

Palavras-chave

Type 310 stainless steel, stress drop experiments, creep transients.

Type 310 stainless steel, stress drop experiments, creep transients.