scholarly journals Dynamics Problem of Mode III Crack Subjected to Superimpose Uniform Loads

2019 ◽  
Vol 585 ◽  
pp. 012091
Author(s):  
Yuntao Wang ◽  
Nianchun Lü ◽  
Jin Cheng
Keyword(s):  
Mode Iii ◽  
Mode Iii Crack

Gradient elasticity with surface energy: mode-III crack problem

1996 ◽  
Vol 33 (30) ◽  
pp. 4531-4559 ◽  
Author(s):  
I. Vardoulakis ◽  
G. Exadaktylos ◽  
E. Aifantis
Keyword(s):  
Surface Energy ◽  
Crack Problem ◽  
Gradient Elasticity ◽  
Mode Iii ◽  
Mode Iii Crack ◽  
Energy Mode

A special purpose Trefftz-element for mode III crack tip loading

2018 ◽  
Vol 192 ◽  
pp. 210-224 ◽  
Author(s):  
J. Hartmann ◽  
T. Heubrandtner ◽  
K. Kunter ◽  
R. Pippan ◽  
B. Fellner ◽  
...  
Keyword(s):  
Crack Tip ◽  
Mode Iii ◽  
Mode Iii Crack

Mode-III crack kinking under stress-wave loading

Wave Motion ◽  
1982 ◽  
Vol 4 (2) ◽  
pp. 181-190 ◽  
Author(s):  
J.P. Dempsey ◽  
M.-K. Kuo ◽  
J.D. Achenbach
Keyword(s):  
Stress Wave ◽  
Wave Loading ◽  
Mode Iii ◽  
Crack Kinking ◽  
Mode Iii Crack

Complete Crack-Tip Shielding of the Mode III Crack in a Work-Hardening Solid

1991 ◽  
Vol 58 (4) ◽  
pp. 1107-1108 ◽  
Author(s):  
J. Weertman
Keyword(s):  
Stress Intensity Factor ◽  
Stress Intensity ◽  
Intensity Factor ◽  
Work Hardening ◽  
Crack Tip ◽  
Mode Iii ◽  
Mode Iii Crack ◽  
Extension Force ◽  
Crack Tip Shielding ◽  
Dislocation Crack

The crack-tip shielding stress intensity factor L, for the mode III crack in a work-hardening solid is equal to L = - K, where K is the applied stress intensity factor. That is, the crack tip is perfectly shielded. This result is shown two ways: from the dislocation shielding and from the dislocation crack extension force.

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