Dilatancy, shear jamming, and a generalized jamming phase diagram of frictionless sphere packings

Soft Matter ◽  
2021 ◽  
Vol 17 (11) ◽  
pp. 3121-3127
Author(s):  
Varghese Babu ◽  
Deng Pan ◽  
Yuliang Jin ◽  
Bulbul Chakraborty ◽  
Srikanth Sastry

Frictionless packings exhibit dilatancy and shear jamming, contrary to previous expectations, depending crucially on the existence of a “jamming line” above the minimal jamming density (J-Point), and with strikingly different rheological behaviour.

2021 ◽  
Vol 103 (2) ◽  
Author(s):  
Ryotaro Koshoji ◽  
Mitsuaki Kawamura ◽  
Masahiro Fukuda ◽  
Taisuke Ozaki

Soft Matter ◽  
2014 ◽  
Vol 10 (39) ◽  
pp. 7838-7848 ◽  
Author(s):  
Vasili Baranau ◽  
Ulrich Tallarek

2020 ◽  
Vol 117 (19) ◽  
pp. 10203-10209 ◽  
Author(s):  
Pallabi Das ◽  
H. A. Vinutha ◽  
Srikanth Sastry

Self-organization, and transitions from reversible to irreversible behavior, of interacting particle assemblies driven by externally imposed stresses or deformation is of interest in comprehending diverse phenomena in soft matter. They have been investigated in a wide range of systems, such as colloidal suspensions, glasses, and granular matter. In different density and driving regimes, such behavior is related to yielding of amorphous solids, jamming, memory formation, etc. How these phenomena are related to each other has not, however, been much studied. In order to obtain a unified view of the different regimes of behavior, and transitions between them, we investigate computationally the response of soft-sphere assemblies to athermal cyclic-shear deformation over a wide range of densities and amplitudes of shear deformation. Cyclic-shear deformation induces transitions from reversible to irreversible behavior in both unjammed and jammed soft-sphere packings. Well above the minimum isotropic jamming density (ϕJ), this transition corresponds to yielding. In the vicinity of the jamming point, up to a higher-density limit, we designate ϕJcyc, an unjammed phase emerges between a localized, absorbing phase and a diffusive, irreversible, phase. The emergence of the unjammed phase signals the shifting of the jamming point to higher densities as a result of annealing and opens a window where shear jamming becomes possible for frictionless packings. Below ϕJ, two distinct localized states, termed point- and loop-reversible, are observed. We characterize in detail the different regimes and transitions between them and obtain a unified density-shear amplitude phase diagram.


2011 ◽  
Vol 107 (12) ◽  
Author(s):  
Adam B. Hopkins ◽  
Yang Jiao ◽  
Frank H. Stillinger ◽  
Salvatore Torquato

1993 ◽  
Vol 90 ◽  
pp. 249-254 ◽  
Author(s):  
C Wolverton ◽  
M Asta ◽  
S Ouannasser ◽  
H Dreyssé ◽  
D de Fontaine

1993 ◽  
Vol 90 ◽  
pp. 175-180 ◽  
Author(s):  
Li Lin ◽  
L Delaey ◽  
P Wollants ◽  
O Van Der Biest

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