Impurities in nematic liquid crystal samples inducing changes in the DSM1-DSM2 transition phase diagram

2000 ◽  
Vol 27 (2) ◽  
pp. 277-281 ◽  
Author(s):  
D. E. Lucchetta ◽  
N. Scaramuzza ◽  
G. Strangi ◽  
C. Versace
Soft Matter ◽  
2019 ◽  
Vol 15 (19) ◽  
pp. 3914-3922 ◽  
Author(s):  
Zeynep Sumer ◽  
Alberto Striolo

In an attempt to bridge the gap between computational and experimental studies, coarse-grained simulations are used to study nematic Liquid Crystal (LC) nanodroplets dispersed in water. A LC phase diagram is generated as a function of droplet size and temperature, and the effect of adding surfactants is quantified.


1998 ◽  
Vol 31 (20) ◽  
pp. 6806-6812 ◽  
Author(s):  
Domasius Nwabunma ◽  
Kap Jin Kim ◽  
Yuhui Lin ◽  
L. C. Chien ◽  
Thein Kyu

1999 ◽  
Vol 559 ◽  
Author(s):  
D. Nwabunma ◽  
T. Kyu ◽  
R.T. Pogue ◽  
T.J. Bunning

ABSTRACTThe influence of elasticity on the phase behavior of a mixture of nematic liquid crystal (LC) and in-situ cross-linked polymer has been investigated. Unlike the phase diagram of the LC/pre-cured polymer, the experimental diagram of LC/cross-linked polymer phase supported by theoretical calculation showed no critical point. Instead, the binodal curve exhibits an upward asymptotic behavior as the LC volume fraction approaches unity due to domination arising from network elasticity, particularly at high LC volume fraction. An examination of the effect of cross-links segment length and network functionality on the phase diagram of LC/cross-linked polymer showed that the segment length between cross-links exerts a greater influence.


1996 ◽  
Vol 10 (23n24) ◽  
pp. 2973-2981 ◽  
Author(s):  
Yun Zhu ◽  
M.L. Ivey ◽  
P. Sheaffer ◽  
J. Pousset ◽  
Jing Liu

Two field-induced phase transition regimes are found in a ferrofluid emulsion system, which are defined by three critical fields, Hc1<HC2<Hc3. The first regime, which starts at Hc1 and finishes at Hc2, is the transition from a gas to induced Nematic liquid crystal phase. In the second regime, or Hc2<H<Hc3, induced Nematic liquid crystal transits to columnar solid structure. A phase diagram is drawn and is explained well by a scaling calculation, which gives Hc1~Φ−1/2, Hc2~Φ−1/4, and Hc3~Φγ exp (πG/Φγ/2), where Φ is the volume fraction, γ=0.172 and G=1.44.


2008 ◽  
Vol 59 (2) ◽  
pp. 181-184
Author(s):  
Cristina Miron

Electroconvection patterns have been studied in a homeotropic nematic liquid crystal, experimental and theoretical, with unusual combination of material parameters, negative conductivity and positive dielectric permittivity anisotropies. Exploring the complete phase diagram in the (U, q) space three distinct morphologies, rolls and squares, soft squares and hard squares have been identified. We perform a linear and nonlinear analysis of the full nematohydrodynamic equations and carry out simulations of a suitably constructed Lorenz model. We obtain in agreement with the experiments modulated rolls and squares at threshold.


2005 ◽  
Vol 38 (11) ◽  
pp. 4844-4854 ◽  
Author(s):  
Scott Meng ◽  
Thein Kyu ◽  
Lalgudi V. Natarajan ◽  
Vincent P. Tondiglia ◽  
Richard L. Sutherland ◽  
...  

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