Tension and Compression Behavior of Axially Loaded Members

Author(s):  
Xianglin Gu ◽  
Xianyu Jin ◽  
Yong Zhou
2020 ◽  
Vol 41 (6) ◽  
pp. 2455-2465
Author(s):  
Liang Shuangqiang ◽  
Zhou Qihong ◽  
Chen Ge ◽  
Frank Ko

2017 ◽  
Vol 2017.30 (0) ◽  
pp. 308
Author(s):  
Toru TSUDA ◽  
Atsushi ABE ◽  
Kouji MIMURA ◽  
Isamu RIKU ◽  
Takashi NUMATA ◽  
...  

2017 ◽  
Vol 43 (15) ◽  
pp. 11635-11641 ◽  
Author(s):  
Tao Fu ◽  
Xianghe Peng ◽  
Cheng Huang ◽  
Shayuan Weng ◽  
Yinbo Zhao ◽  
...  

2013 ◽  
Vol 50 ◽  
pp. 702-712 ◽  
Author(s):  
F. Fereshteh-Saniee ◽  
Kh. Fallah-Nejad ◽  
A.Sh. Beheshtiha ◽  
H. Badnava

2008 ◽  
Vol 49 (564) ◽  
pp. 76-81 ◽  
Author(s):  
Toshihiko KUWABARA ◽  
Yutaka KUMANO ◽  
Jindra ZIEGELHEIM ◽  
Ikuya KUROSAKI

1993 ◽  
Vol 322 ◽  
Author(s):  
Amit K. Ghosh ◽  
Ajoy Basu

AbstractMonolithic MoSi2 and MoSi2 reinforced with SiC particulate reinforcements have been produced with widely varying grain sizes. Monotonic compression behavior of these materials has been examined in the temperature range of room temperature to 1200°C. Based on these results, the ductile-to-brittle transition temperature at low deformation rate of MoSi2 and its composite appears to be near 900°C and may decrease slightly with decreasing grain size. Tension and compression creep behavior of these materials were also studied between 1100 and 1400°C. Creep strength of the matrix decreases with decreasing grain size even in the nominally dislocation climb-glide regime. While 20 vol% SiC particulates provide a reasonable amount of creep strengthening of the fine grain MoSi2 matrix, strengthening due to coarser grain size can be significantly higher in these materials. These results parallel those on other intermetallics.


2017 ◽  
Vol 39 (4) ◽  
pp. 375-386
Author(s):  
Christian Lexcellent

Depending of the shape of the crack tip e.g. with or without curvature, the size of the phase transformation surface between a mother phase A (austenite) and a producted phase M (martensite) is different. The presentation is focussed to the modes I and II (opening and shearing modes). The elastic stress field around the crack tip without curvature is known in the litterature and the use of Linear Elastic Mechanical Theory is consistent with the deformations amplitude associated the beginning of the phase transformation (A \(\Rightarrow\) M). In order to take into account the curvature at the crack tip, one uses the approximated expressions of Creager and Paris (1967). A special attention is devoted to take into account the asymmetry between tension and compression behavior in the surfaces prediction.


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