Dispersion characteristics and rheology of organoclay nanocomposites based on a segmented main-chain liquid-crystalline polymer having side-chain azopyridine with flexible spacer

Polymer ◽  
2006 ◽  
Vol 47 (12) ◽  
pp. 4400-4410 ◽  
Author(s):  
Wenyi Huang ◽  
Chang Dae Han

2016 ◽  
Vol 49 (19) ◽  
pp. 7238-7245 ◽  
Author(s):  
Ping-Ping Hou ◽  
Zhen-Yu Zhang ◽  
Qian Wang ◽  
Meng-Yao Zhang ◽  
Zhihao Shen ◽  
...  






RSC Advances ◽  
2015 ◽  
Vol 5 (86) ◽  
pp. 70163-70171 ◽  
Author(s):  
Ping-Ping Hou ◽  
Ke-Hua Gu ◽  
Yu-Feng Zhu ◽  
Zheng-Yu Zhang ◽  
Qian Wang ◽  
...  

A polynorbornene-based mesogen-jacketed liquid crystalline polymer containing side-chain crystalline POSS moieties was synthesized through ROMP. It self-assembles into an organic–inorganic hybrid inclusion complex on the sub-10 nm scale.



RSC Advances ◽  
2015 ◽  
Vol 5 (118) ◽  
pp. 97187-97194 ◽  
Author(s):  
He-lou Xie ◽  
Bin Ni ◽  
Quan Liu ◽  
Jun Wang ◽  
Shuang Yang ◽  
...  

A series of combined main-chain/side-chain liquid crystalline polymers based on the “jacketing” effect, with different alkyl spacer lengths (n = 2–10), have been successfully synthesized and their self-organization behavior has been investigated.



Cellulose ◽  
2010 ◽  
Vol 17 (3) ◽  
pp. 547-558 ◽  
Author(s):  
Tianhui Hu ◽  
Helou Xie ◽  
Jianbo Xiao ◽  
Hailiang Zhang ◽  
Erqiang Chen




1999 ◽  
Vol 32 (2) ◽  
pp. 521-523 ◽  
Author(s):  
Iwhan Cho ◽  
Su-Yeon Jo


MRS Bulletin ◽  
1995 ◽  
Vol 20 (9) ◽  
pp. 39-41 ◽  
Author(s):  
David R.M. Williams ◽  
Avi Halperin

Conventionally, the term “defects” in liquid-crystalline systems refers to microscopic faults in the orientational order, which are usually visible optically. These are discussed in other articles in this issue. Our use of the term defect is entirely different. The defects we shall be considering, “hairpins,” occur on the scale of several angstroms and are abrupt reversals in the trajectory of a single liquid-crystalline-polymer (LCP) chain (Figure 1). In comparison to conventional defects, the direct observation of hairpin defects is much more difficult, yet their presence has important effects. Among the affected properties are the dimensions and the elasticity of the chains, the elastic behavior of the bulk nematic, and its dielectric response. Their presence should also give rise to a family of interfacial phase transitions in solutions of LCPs in nematic solvents. In turn, these are of interest in the design of liquid-crystalline displays. Hairpins in LCPs are superficially reminiscent of similar configurations in proteins and in homopolymers that undergo fold crystallization. These similarities are misleading because hairpins in proteins are permanent structures due to the chemical bonds. The folds in crystalline polymers are also fixed structures. In marked contrast, hairpin defects are mobile topological excitations that are created and annihilated continuously. Our emphasis in this article is on main-chain, semiflexible, nematic LCPs, consisting of mesogenic monomers joined by flexible spacer chains (Figure la). These polymers combine the orientational order of monomeric nematics with the flexibility and randomness inherent in polymers. The appearance of an oriented, nematic phase can be controlled either by temperature or by concentration.



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