Fluctuations of a cholesteric liquid crystal in a static magnetic field

1974 ◽  
Vol 9 (6) ◽  
pp. 2652-2656 ◽  
Author(s):  
J. D. Parsons ◽  
Charles F. Hayes
Author(s):  
G. Paria ◽  
A. K. Sharma

AbstractThe paper investigates the effect of a static magnetic field on the helical flow of an incompressible cholestenc liquid crystal with director of unit magnitude between two coaxial circular cylinders rotating with different angular velocities about their common axis and moving with different axial velocities. At low shear rates with a weak magnetic field in the axial direction, the axial velocity, the angular velocity and the orientation of molecules between the two cylinders have been obtained. It is found that the magnetic field has influenced the orientation of molecules while the axial velocity and the angular velocity remain uneffected by the magnetic field.


1969 ◽  
Vol 51 (10) ◽  
pp. 4186-4188 ◽  
Author(s):  
Thomas M. Laronge ◽  
H. Baessler ◽  
M. M. Labes

2019 ◽  
Vol 84 (4) ◽  
pp. 748-762
Author(s):  
Carlo Greco

Abstract In a thin layer of liquid crystal the configuration of the director field depends on the interaction between the elastic properties of the material, the thickness $d$ of the layer, the boundary conditions and the external fields that may have been applied. Suitable combinations of these factors can give rise to distorted configurations (Freedericksz transitions). In this paper we assume the Oseen-Frank model for the energy and that the director field depends only on the direction orthogonal to the layer; we assume also weak anchoring conditions at the two bounding surfaces, and we mainly study the problem of uniqueness of such distorted configurations. More precisely, we first consider the nematic case in the presence of a magnetic field $\mathbf H$, and we prove the uniqueness of the stable configuration provided the magnitude of $\mathbf H$ is between two critical thresholds, simplifying some results already known in the literature, and calculating explicitly the critical thresholds. Then we study the case of a cholesteric liquid crystal without external field. In this case the director field tends to form a right-angle helicoid around a twist axis orthogonal to the layer, and we have distorted configurations (namely oblique helicoid) for suitable value of $d$. Also in this case, with suitable restrictions on the elastic constants in the Oseen-Frank energy, we find two critical thresholds for $d$, and we prove the existence of only one stable director configuration if $d$ is between them.


Open Physics ◽  
2012 ◽  
Vol 10 (3) ◽  
Author(s):  
Ioannis Lelidis ◽  
Giovanni Barbero ◽  
Antonio Scarfone

AbstractWe investigate the pitch transitions induced by an external bulk field in a Cholesteric Liquid Crystal slab of finite thickness ℓ that contains an incomplete number of π-twists. The analysis is performed for a magnetic field that is (i) perpendicular to the helical axis, and (ii) tilted with respect to one of the easy directions imposed by planar and rigid boundary conditions. For finite ℓ we obtain a cascade of transitions, where the bulk expels a half-pitch at a time with increasing field to avoid divergences in the elastic energy. The dependence of the threshold magnetic field inducing the expulsion on the easy axes twist angle δ is investigated for all the cascade of pitch transitions and in particular for the final one, corresponding to the Cholesteric-Nematic transition. In the ℓ → ∞ limit this dependence disappears and we reobtain the results of de Gennes for an infinite sample.


2020 ◽  
Vol 11 (1) ◽  
pp. 171
Author(s):  
Shi-Tong Xu ◽  
Fei Fan ◽  
Shu Chen ◽  
Yanzhao Xing ◽  
Yuebo Gao ◽  
...  

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