Shear jamming onset in dense granular suspensions

2021 ◽  
Vol 65 (3) ◽  
pp. 419-426
Author(s):  
Saisai Cao ◽  
Yu Wang ◽  
Haoming Pang ◽  
Junshuo Zhang ◽  
Yuxuan Wu ◽  
...  
2022 ◽  
Vol 66 (2) ◽  
pp. 237-256
Author(s):  
C. Garat ◽  
S. Kiesgen de Richter ◽  
P. Lidon ◽  
A. Colin ◽  
G. Ovarlez

2017 ◽  
Vol 95 (1) ◽  
Author(s):  
Sayantan Majumdar ◽  
Ivo R. Peters ◽  
Endao Han ◽  
Heinrich M. Jaeger

Soft Matter ◽  
2014 ◽  
Vol 10 (18) ◽  
pp. 3277 ◽  
Author(s):  
B. Haffner ◽  
Y. Khidas ◽  
O. Pitois
Keyword(s):  

2014 ◽  
pp. 467-472
Author(s):  
L Amarsid ◽  
P Mutabaruka ◽  
J Delenne ◽  
Y Monerie ◽  
F Radjai

2018 ◽  
Vol 4 (3) ◽  
pp. eaar3296 ◽  
Author(s):  
Christopher Ness ◽  
Romain Mari ◽  
Michael E. Cates
Keyword(s):  

2011 ◽  
Vol 172-174 ◽  
pp. 1106-1111 ◽  
Author(s):  
Nicolas Rivier ◽  
Jean Yves Fortin

Dry granular matter, with infinite tangential friction, is modeled as a connected graph ofgrains linked by purely repulsive contacts. The degrees of freedom of a grain are non-slip rotationon, and disconnection from another. The material stability under shear (jamming) is ensured by oddcircuits of grains in contact that prevent the grains from rolling on each other. A dense granularmaterial with high stiffness-to-load ratio has two possible states: fragile solid, blocked by odd circuits,and dry fluid or bearing, in the absence of odd circuits, that flows under shear by creation and glide ofa pair of dislocations as in plasticity of continuous media. In this paper, we introduce the notions of blob, a region of the material containing only even circuits, and of critical contact that closes an oddcircuit. The granular material is then represented, at low energies and critical applied shear, as a chainof blobs connected by critical contacts. The transition between dry fluid and fragile solid occurs byintermittency.


2020 ◽  
Vol 125 (7) ◽  
Author(s):  
Christopher Madec ◽  
Brivaël Collin ◽  
J. John Soundar Jerome ◽  
Sylvain Joubaud

2019 ◽  
Vol 122 (16) ◽  
Author(s):  
Nariaki Sakaï ◽  
Sébastien Moulinet ◽  
Frédéric Lechenault ◽  
Mokhtar Adda-Bedia

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