scholarly journals Oscillatory shear-induced 3D crystalline order in colloidal hard-sphere fluids

Soft Matter ◽  
2012 ◽  
Vol 8 (26) ◽  
pp. 6931 ◽  
Author(s):  
T. H. Besseling ◽  
M. Hermes ◽  
A. Fortini ◽  
M. Dijkstra ◽  
A. Imhof ◽  
...  
Soft Matter ◽  
2020 ◽  
Vol 16 (43) ◽  
pp. 9864-9875
Author(s):  
Young Ki Lee ◽  
Kyu Hyun ◽  
Kyung Hyun Ahn

The first normal stress difference (N1) as well as shear stress of non-Brownian hard-sphere suspensions in small to large amplitude oscillatory shear flow is investigated.


2002 ◽  
Vol 66 (5) ◽  
Author(s):  
G. Petekidis ◽  
A. Moussaïd ◽  
P. N. Pusey

1997 ◽  
Vol 92 (2) ◽  
pp. 211-228 ◽  
Author(s):  
R.J. F. LEOTE DE CARVALHO ◽  
R. EVANS
Keyword(s):  

1998 ◽  
Vol 95 (2) ◽  
pp. 131-135 ◽  
Author(s):  
DOUGLAS HENDERSON DEZSO BODA KWONG-YU CHAN
Keyword(s):  

1998 ◽  
Vol 77 (5) ◽  
pp. 1441-1447
Author(s):  
S. Rabinovich, E. Brook-Levinson, E. Z

2019 ◽  
Author(s):  
Shengxian Cheng ◽  
Xiaoxia Ma, ◽  
Yonghe He ◽  
Jun He ◽  
Matthias Zeller ◽  
...  

We report a curious porous molecular crystal that is devoid of the common traits of related systems. Namely, the molecule does not rely on directional hydrogen bonds to enforce open packing; and it offers neither large concave faces (i.e., high internal free volume) to frustrate close packing, nor any inherently built-in cavity like in the class of organic cages. Instead, the permanent porosity (as unveiled by the X-ray crystal structure and CO<sub>2</sub> sorption studies) arises from the strong push-pull units built into a Sierpinski-like molecule that features four symmetrically backfolded (<b>SBF</b>) side arms. Each side arm consists of the 1,1,4,4-tetracyanobuta-1,3-diene acceptor (TCBD) coupled with the dimethylaminophenyl donor, which is conveniently installed by a cycloaddition-retroelectrocyclization (CA-RE) reaction. Unlike the poor/fragile crystalline order of many porous molecular solids, the molecule here readily crystallizes and the crystalline phase can be easily deposited into thin films from solutions. Moreover, both the bulk sample and thin film exhibit excellent thermal stability with the porous crystalline order maintained even at 200 °C. The intermolecular forces underlying this robust porous molecular crystal likely include the strong dipole interactions and the multiple C···N and C···O short contacts afforded by the strongly donating and accepting groups integrated within the rigid molecular scaffold.


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