Pressure-volume-temperature relations of liquid, crystal, and glass of o-terphenyl: excess amorphous entropies, and factors determining molecular mobility

1989 ◽  
Vol 93 (2) ◽  
pp. 948-955 ◽  
Author(s):  
Motosuke Naoki ◽  
Susumu Koeda
1999 ◽  
Vol 41 (5) ◽  
pp. 777-779
Author(s):  
E. A. Egorov ◽  
A. V. Savitskii ◽  
V. V. Zhizhenkov ◽  
I. A. Gorshkova

Soft Matter ◽  
2020 ◽  
Vol 16 (8) ◽  
pp. 2005-2016 ◽  
Author(s):  
Arda Yildirim ◽  
Christina Krause ◽  
Reiner Zorn ◽  
Wiebke Lohstroh ◽  
Gerald J. Schneider ◽  
...  

The molecular mobility of the discotic liquid crystal HAT6 is investigated in a broad time range using different methods.


2020 ◽  
Vol 47 (8) ◽  
pp. 1180-1194 ◽  
Author(s):  
Alfonso Martinez-Felipe ◽  
Thamil Selvi Velayutham ◽  
Nurul Fadhilah Kamalul Aripin ◽  
Marina Yusoff ◽  
Emma Farquharson ◽  
...  

2018 ◽  
Vol 122 (29) ◽  
pp. 7409-7415 ◽  
Author(s):  
Sho Nakagami ◽  
Takuya Akita ◽  
Daichi Kiyohara ◽  
Yoshiaki Uchida ◽  
Rui Tamura ◽  
...  

Author(s):  
K.J. Ihn ◽  
R. Pindak ◽  
J. A. N. Zasadzinski

A new liquid crystal (called the smectic-A* phase) that combines cholesteric twist and smectic layering was a surprise as smectic phases preclude twist distortions. However, the twist grain boundary (TGB) model of Renn and Lubensky predicted a defect-mediated smectic phase that incorporates cholesteric twist by a lattice of screw dislocations. The TGB model for the liquid crystal analog of the Abrikosov phase of superconductors consists of regularly spaced grain boundaries of screw dislocations, parallel to each other within the grain boundary, but rotated by a fixed angle with respect to adjacent grain boundaries. The dislocations divide the layers into blocks which rotate by a discrete amount, Δθ, given by the ratio of the layer spacing, d, to the distance between grain boundaries, lb; Δθ ≈ d/lb (Fig. 1).


Author(s):  
B.D. Terris ◽  
R. J. Twieg ◽  
C. Nguyen ◽  
G. Sigaud ◽  
H. T. Nguyen

We have used a force microscope in the attractive, or noncontact, mode to image a variety of surfaces. In this mode, the microscope tip is oscillated near its resonant frequency and shifts in this frequency due to changes in the surface-tip force gradient are detected. We have used this technique in a variety of applications to polymers, including electrostatic charging, phase separation of ionomer surfaces, and crazing of glassy films.Most recently, we have applied the force microscope to imaging the free surfaces of chiral liquid crystal films. The compounds used (Table 1) have been chosen for their polymorphic variety of fluid mesophases, all of which exist within the temperature control range of our force microscope.


Sign in / Sign up

Export Citation Format

Share Document