| 1. |
Effects of Hydrogen Charge on Fatigue Strength of Stainless Steels
The effect of hydrogen on fatigue strength of stainless steels was investigated. There were no definite differences in fatigue life of unnotched specimens between hydrogen-charged specimen (2.46.4 ppm) and uncharged specimen (2.2ppm) of SUS 304. High content of hydrogen (10100 ppm) was detected in a very thin surface layer, approximately at 100200 μm from specimen surface of SUS 304 specimens hydrogen-charged for 336672 hours. There were also no definite differences in fatigue life of unnotched specimens between hydrogen-charged specimen (1.85.8 ppm) and uncharged specimen (0.1ppm) of SUS 405. The uncharged specimens of 0.7 C13 Cr steel (0.2 ppm) failed from subsurface non-metallic inclusions in surface layer. ODAs (Optically Dark Area) were not observed due to the tensile residual stress in the surface layer although the specimens failed in the high cycle regime of 10<SUP>7</SUP> cycles. Increasing hydrogen content from 0.2 ppm to 2.42.7 ppm, the fatigue strength and fatigue life were markedly decreased in 0.7 C13 Cr steel.. |
| 2. |
Effects of hydrogen charge on fatigue strength of stainless steels
The effect of hydrogen on fatigue strength of stainless steels was investigated. There were no definite differences in fatigue life of unnotched specimens between hydrogen-charged specimen (2.4-6.4ppm) and uncharged specimen (2.2ppm) of SUS 304. High content of hydrogen (10-100 ppm) was detected in a very thin surface layer, approximately at 100-200 (im from specimen surface of SUS 304 specimens hydrogen-charged for 336-672 hours. There were also no definite differences in fatigue life of unnotched specimens between hydrogen-charged specimen (1.8-5.8ppm) and uncharged specimen (0.1 ppm) of SUS 405. The uncharged specimens of 0.7 C-13 Cr steel (0.2 ppm) failed from subsurface non-metallic inclusions in surface layer. ODAs (Optically Dark Area) were not observed due to the tensile residual stress in the surface layer although the specimens failed in the high cycle regime of 107 cycles. Increasing hydrogen content from 0.2 ppm to 2.4-2.7 ppm, the fatigue strength and fatigue life were markedly decreased in 0.7C-13Cr steel.. |
| 3. |
Threshold of shear-mode fatigue crack growth in bearing steel
Semi-elliptical shear-mode fatigue cracks were studied in SAE52100 bearing steel loaded with fully-reversed cyclic torsion combined with a static axial compressive stress. Non-propagating cracks smaller than 1 mm in length were obtained in the following two ways; (i) decreasing stress amplitude tests using notched specimens, and (ii) constant stress amplitude tests using smooth specimens. The shape and dimensions of the non-propagating cracks were investigated by a successive polishing of the specimen surface, and the threshold stress intensity factor ranges, δK IIth and δK IIIth, were estimated. The threshold values decreased with a decrease in crack size. There was no significant difference between δK IIth and δK IIIth. Wear on the crack surfaces during crack-growth was inferred by a change in microstructure.. |
| 4. |
A. J. McEvily, H. Matsunaga, On Fatigue Striations, SCIENTIA IRANICA TRANSACTION B-MECHANICAL ENGINEERING, Vol.17, No.1, pp.75-82, 2010.01, This paper provides a review of the research that has led to our current understanding of the process of fatigue striation formation. An important question addressed is whether or not at low stress intensity values, fatigue cracks can propagate intermittently in steels and aluminum alloys. It is concluded that there is no valid evidence for propagation, on other than a cycle-by-cycle basis.. |
| 5. |
H. Matsunaga, N. Shomura, S. Muramoto, M. Endo, Shear mode threshold for a small fatigue crack in a bearing steel, FATIGUE & FRACTURE OF ENGINEERING MATERIALS & STRUCTURES, 10.1111/j.1460-2695.2010.01495.x, Vol.34, No.1, pp.72-82, 2011.01, The fatigue behaviour of small, semi-elliptical surface cracks in a bearing steel was investigated under cyclic shear-mode loading in ambient air. Fully reversed torsion was combined with a static axial compressive stress to obtain a stable shear-mode crack growth in the longitudinal direction of cylindrical specimens. Non-propagating cracks less than 1 mm in size were obtained (i) by decreasing the stress amplitude in tests using notched specimens and (ii) by using smooth specimens in constant stress amplitude tests. The threshold stress intensity factor ranges, delta K(IIth) and delta K(IIIth), were estimated from the shape and dimensions of non-propagating cracks. Wear on the crack faces was inferred by debris and also by changes in microstructure in the wake of crack tip. These effects resulted in a significant increase in the threshold value. The threshold value decreased with a decrease in crack size. No significant difference was observed between the values of delta K(IIth) and delta K(IIIth).. |
| 6. |
Yanase Keiji, Endo Masahiro, Matsunaga Hisao, OS12-3-2 Prediction for Fatigue Crack Behavior under Biaxial Loading, Abstracts of ATEM : International Conference on Advanced Technology in Experimental Mechanics : Asian Conference on Experimental Mechanics, Vol.2011, No.10, pp."OS12-3-2-1", 2011.09. |
| 7. |
H. Matsunaga, C. Sun, Y. Hong, Y. Murakami, Dominant factors for very-high-cycle fatigue of high-strength steels and a new design method for components, Fatigue and Fracture of Engineering Materials and Structures, 10.1111/ffe.12331, Vol.38, No.11, pp.1274-1284, 2015.11, © 2015 Wiley Publishing Ltd. Dominant factors affecting fatigue failure from non-metallic inclusions in the very-high-cycle fatigue (VHCF) regime are reviewed, and the mechanism for the disappearance of the conventional fatigue limit is discussed. Specifically, this paper focuses on the following: (i) the crucial role of internal hydrogen trapped by non-metallic inclusions for the growth of the optically dark area (around the non-metallic inclusion at fracture origin), (ii) the behaviour of the crack growth from a non-metallic inclusion as a small crack and (iii) the statistical aspects of the VHCF strength, in consideration of the maximum inclusion size, using statistics of extremes. In addition, on the basis of the aforementioned findings, a new fatigue design method is proposed for the VHCF regime. The design method gives the allowable stress, σallowable, for a determined design life, NfD, as the lower bound of scatter of fatigue strength, which depends on the amount of components produced.. |
| 8. |
Analysis on Fatigue Life and its Scatter of Specimens Containing Small Artificial Defects with Various Sizes Based on the Essential Structure of S-N Curve
The origin of fatigue life scatter was quantitatively analyzed by fatigue test of specimens containing small drill holes with various sizes. The size of the holes ranged from 40 µm to 400 µm. In several specimens, three holes with different sizes were introduced to investigate the behavior of crack growth from holes which were observed at the cycle Nf of fatigue failure from the largest hole. The dependency of fatigue life and its scatter on defect size and stress level was analyzed by the model explained in the 1st report and the factors which cause the scatter of fatigue life for other materials such as cast irons and AM materials were discussed by comparing the fatigue data and the predictions.. |
| 9. |
Essential Structure of S-N Curve and the Essence of Scatter of Fatigue Life
Historically, S-N curve has been expressed in the form of an exponential relationship between applied stress σ and number of cycles to failure Nf regardless of scatter of data. This paper elucidates the essential structure of S-N curve and the causes of scatter of fatigue life and fatigue limit based on the prediction model for materials containing various defects. The validity of the model was verified by testing specimens containing small defects with various sizes and by analyzing the difference of failure lives due to defect size. The model was successfully applied to the data reported by other researchers. It was revealed that the statistical nature of the scatter of fatigue data should be expressed by the statistics of extremes, because the source of the scatter is originated from the largest defect contained in specimens.. |
| 10. |
Fracture Mechanics-Based Criteria for Fatigue Fracture of Rolling Bearings under the Influence of Defects. |
| 11. |
Yukitaka MURAKAMI, Hisao MATSUNAGA, Ryuichi EZAKI, Measurement of residual stress distribution in a micro-indentation on Ti-6Al-4V alloy, SPring-8 User Experiment Report (JASRI), 2003A, p.71, 2003.11. |
| 12. |
Yukitaka MURAKAMI, Hisao MATSUNAGA, Tohru UEDA, Ryuichi EZAKI, Measurement of residual stress distribution in a micro-indentation on Ti-6Al-4V alloy, SPring-8 User Experiment Report (JASRI), 2002B, p.60, 2003.06. |
| 13. |
Yukitaka MURAKAMI, Tohru UEDA, Hisao MATSUNAGA, X-Ray Diffraction of Hydrogen Charged and Uncharged Cr-Mo Steel SCM435, SPring-8 User Experiment Report (JASRI), 2002A, p.31, 2002.10. |
| 14. |
Yukitaka MURAKAMI, Katsuyuki KANENAWA, Hisao MATSUNAGA, Ryuichi EZAKI, Measurement of residual stress distribution in a micro-indentation on Ti-6Al-4V alloy, SPring-8 User Experiment Report (JASRI), 2002A, p.70, 2002.10. |
| 15. |
Yukitaka MURAKAMI, Yoshihiro FUKUSHIMA, Katsuyuki KANENAWA, Hisao MATSUNAGA, Ryuichi EZAKI, Measurement of residual stress distribution in a micro-indentation on Ti-6Al-4V alloy, SPring-8 User Experiment Report (JASRI), 2001B, p.83, 2002.05. |
| 16. |
Yukitaka MURAKAMI, Yoshihiro FUKUSHIMA, Hisao MATSUNAGA, Measurement of residual stress distribution in a micro-indentation on Ti-6Al-4V alloy, SPring-8 User Experiment Report (JASRI), 2001A, p.80, 2001.10. |
