Constraint Effects in Fracture Theory and Applicatons: Second Volume

1999 ◽  
Vol 15 (3) ◽  
pp. 275-284 ◽  
Author(s):  
C Thaulow ◽  
Z.L Zhang ◽  
M Hauge ◽  
W Burget ◽  
D Memhard

1960 ◽  
Vol 27 (2) ◽  
pp. 352-353 ◽  
Author(s):  
J. L. Sanders
Keyword(s):  

2021 ◽  
Vol 125 ◽  
pp. 107425
Author(s):  
Shengkun Li ◽  
Xiaobing Li ◽  
Huashun Dou ◽  
Dongliang Dang ◽  
Jirui Gong

2014 ◽  
Vol 51 (6) ◽  
pp. 1311-1321 ◽  
Author(s):  
Guian Qian ◽  
V.F. Gonzalez-Albuixech ◽  
Markus Niffenegger

2019 ◽  
Vol 10 (1) ◽  
pp. 253-273 ◽  
Author(s):  
Ilya Svetlizky ◽  
Elsa Bayart ◽  
Jay Fineberg

Contacting bodies subjected to sufficiently large applied shear will undergo frictional sliding. The onset of this motion is mediated by dynamically propagating fronts, akin to earthquakes, that rupture the discrete contacts that form the interface separating the bodies. Macroscopic motion commences only after these ruptures have traversed the entire interface. Comparison of measured rupture dynamics with the detailed predictions of fracture mechanics reveals that the propagation dynamics, dissipative properties, radiation, and arrest of these “laboratory earthquakes” are in excellent quantitative agreement with the predictions of the theory of brittle fracture. Thus, interface fracture replaces the idea of a characteristic static friction coefficient as a description of the onset of friction. This fracture-based description of friction additionally provides a fundamental description of earthquake dynamics and arrest.


2005 ◽  
Vol 53 (9) ◽  
pp. 1951-1983 ◽  
Author(s):  
T. Pardoen ◽  
T. Ferracin ◽  
C.M. Landis ◽  
F. Delannay

2017 ◽  
Vol 18 (3) ◽  
pp. 381-393
Author(s):  
Viktor Michajlovich Markochev ◽  
Mikhail Ivanovich Alymov

Sign in / Sign up

Export Citation Format

Share Document