compressive hold
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2017 ◽  
Vol 104 ◽  
pp. 61-71 ◽  
Author(s):  
Run-Zi Wang ◽  
Xu-Min Zhu ◽  
Xian-Cheng Zhang ◽  
Shan-Tung Tu ◽  
Jian-Guo Gong ◽  
...  

2017 ◽  
Vol 40 (9) ◽  
pp. 1406-1415 ◽  
Author(s):  
A. T. Radzicki ◽  
W. S. Johnson ◽  
R. W. Neu ◽  
B. S. Annigeri ◽  
B. M. Ziegler

2016 ◽  
pp. 959-967 ◽  
Author(s):  
Swapnil Patil ◽  
Shenyan Huang ◽  
Mallikarjun Karadge ◽  
Doug Konitzer ◽  
Akane Suzuki

2013 ◽  
Vol 592-593 ◽  
pp. 429-432
Author(s):  
Miroslav Šmíd ◽  
Karel Obrtlík

The present paper is focused on scanning electron microscopy investigation of surface relief developed in cyclically strained specimens at high temperature. Symmetrical fatigue tests without hold times and with tensile or compressive hold times were used in strain control regime. The gauge length of specimens was analyzed after cyclic straining in a wide range of total strain amplitudes. Experimental temperature was 800 °C and selected hold time was 10 minutes.Surface relief is developed during the cyclic straining in localized plastic strain areas. Developed surface relief strongly depends on the type of fatigue test and a value of total strain amplitude. Well-developed surface persistent slip markings were observed after cyclic loading without hold times. Another group of observed slip markings with perpendicular orientation to stress axis exhibits irregular and wavy morphology. Similar markings were also observed on specimen surfaces after fatigue tests with tensile hold times as well as compressive hold times. Third group, named imperfect persistent slip markings, was observed after cyclic straining with tensile holds. In some suitably oriented grains, areas with high density of well-developed markings with irregular morphology were found.


Author(s):  
B. Fournier ◽  
M. Sauzay ◽  
A. Pineau

The 9–12%Cr martensitic steels are candidate materials for several components of the generation IV and fusion nuclear reactors. In these future applications, in addition to long holding periods, cyclic loadings corresponding to start and stopoperations and maintenance must also be taken into account. Creep-fatigue interactions must therefore be considered to design these components. A broad literature review showed that between 20°C and 650°C the fatigue lifetime of these materials followed a unique Manson-Coffin law. Adding a stress-relaxation holding period significantly reduces the fatigue lifetime for total strain lower than Δεt = 0.7%. For higher strain ranges, no significant effect of holding period exists anymore. Moreover, several studies reported a more deleterious effect of compressive hold times compared to tensile holding periods. Additional tests and detailed observations of the damage mechanisms responsible for fracture of pure fatigue, relaxation-fatigue and creep-fatigue tests were carried out on a 9 Cr − 1 Mo modified steel tested at 550°C in air. This material showed a strong work softening effect. The cyclic plastic behavior of the material was studied using an enhanced stress partitioning method to evaluate the kinematic, isotropic and viscous parts of the cyclic stress. It was concluded that in all the cases the observed softening effect was mainly due to the kinematic stress decrease [1]. The effect of a tensile or compressive hold time on fatigue life was also investigated [2, 3]. The deleterious effect of compressive hold times was thus confirmed. No creep cavitation was observed and the fracture was due to the propagation of transgranular fatigue cracks. Two distinct damage mechanisms were identified, depending on the strain range and the hold time : (i) crack initiation occurred due to usual Stage I extrusions/intrusions mechanisms leading to the propagation of a bifurcated crack; (ii) multiple cracks were initiated from the brittle fracture of the oxide layer formed at the free surface of the specimens. It was shown that this oxide failure leads to a penetration of oxygen along the microstructural boundaries enabling the cracks to propagate. Oxide layers grown during tensile (compressive) holding periods are mainly loaded in compression (tension) during the fatigue cycle. The critical strains necessary to crack oxide layers are lower for tensile loading (i.e. compressive holding periods) as shown by finite element and analytical calculations. Therefore compressive holding periods leads more easily to the second and more severe damage mechanism [2, 3]. A model, identified on short crack propagation tests and from experimental endurance curves, gives excellent predictions in pure-fatigue [4]. In creep-fatigue the predicted lifetimes are in the usual range [Nexp/2, 2Nexp] for all strain amplitudes and hold times. In addition, complex phenomena, such as the deleterious effect of compressive holding periods are also reproduced. An attempt is made to show how this model can be extrapolated in temperature to longer hold times.


1991 ◽  
Vol 226 ◽  
Author(s):  
Semyon Vaynhan ◽  
Morris E. Fine

AbstractThis paper discusses the effects of the most important variables during isothermal fatigue such as strain range, ramp time, tensile and compressive hold times, and temperature on fatigue life of near–eutectic 62Sn–36Pb–2Ag solder at strain ranges below 3.0%. The Coffin-Manson relation does not hold for 62Sn–36Pb–2Ag solder below 1% strain range. Decreasing frequency below 10-2 in no-hold tests reduces the number of cycles to failure. Tensile hold time or compressive hold time alone in the cycle dramatically reduce the number of cycles to failure. Increase of hold time over a few minutes leads to saturation of Nf. Combined tensile and compressive hold times affect the fatigue life of this solder less than either tensile or compressive hold alone. The effect of hold times on fatigue life is much stronger than the effect of ramp time. Practically no ramp time effect was observed in tests with tensile hold times. Very little effect of temperature over the range 25 to 80°C on fatigue life of 62Sn–36Pb–2Ag solder was observed when tested at total strain range of 1%.


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