scholarly journals Sol–gel phase transitions in thermoreversible gels: Onset of gelation and melting

1996 ◽  
Vol 105 (2) ◽  
pp. 825-836 ◽  
Author(s):  
Y. Liu ◽  
R. B. Pandey
1986 ◽  
Vol 73 ◽  
Author(s):  
Vered R. Kaufman ◽  
David Avnir

ABSTRACTWhen the polymerization of Si(OCH3)4 is carried out in the presence of surface active agents, prolonged oscillations (over 1000 hrs) at the gel/xerogel transition are observed. The oscillations are of large amplitude, they are slow (several hrs/period), and they exhibit a chaotic behaviour. The probe by which these oscillations are observed is emission from excited state monomeric and excimeric pyrene. It is suggested tentatively that the driving forces for this oscillation are the structural relaxation of the secondary polymeric gel structure and the dispersion of adsorbed pyrene to thermodynamically favored adsorption sites. Relevant models could be those of oscillatory sol/gel phase transitions and of oscillatory polymerization reactions. We are unaware of previous observations of oscillations in sol/gel systems.


2009 ◽  
Vol 9 (10) ◽  
pp. 5990-5996 ◽  
Author(s):  
Soo Jin Lee ◽  
Sung Ho Jung ◽  
Seok-Hoon Lee ◽  
Won Seok Han ◽  
Jong Hwa Jung
Keyword(s):  
Sol Gel ◽  

2020 ◽  
Vol 64 (4) ◽  
pp. 837-850
Author(s):  
Alexander P. Haring ◽  
Manjot Singh ◽  
Miharu Koh ◽  
Ellen Cesewski ◽  
David A. Dillard ◽  
...  

2015 ◽  
Vol 17 (9) ◽  
pp. 6212-6216 ◽  
Author(s):  
Adela I. Carrillo ◽  
Jürgen Bachl ◽  
Judith Mayr ◽  
Pedro J. Plaza-González ◽  
José M. Cátala-Civera ◽  
...  

A non-invasive open coaxial re-entrant microwave sensor allows for the continuous monitoring of sol–gel phase transitions in physical gels.


2000 ◽  
Vol 628 ◽  
Author(s):  
Kazuki Nakanishi ◽  
Souichi Kumon ◽  
Kazuyuki Hirao ◽  
Hiroshi Jinnai

ABSTRACTMacroporous silicate thick films were prepared by a sol-gel dip-coating method accompanied by the phase separation using methyl-trimethoxysilane (MTMS), nitric acid and dimethylformamide (DMF) as starting components. The morphology of the film varied to a large extent depending on the time elapsed after the hydrolysis until the dipping of the coating solution. On a glass substrate, the films prepared by early dipping had inhomogeneous submicrometer-sized pores on the surface of the film. At increased reaction times, relatively narrow sized isolated macropores were observed and their size gradually decreased with the increase of reaction time. On a polyester substrate, in contrast, micrometer-sized isolated spherical gel domains were homogeneously deposited by earlier dippings. With an increase of reaction time, the volume fraction of the gel phase increased, then the morphology of the coating transformed into co-continuous gel domains and macropores, and finally inverted into the continuous gel domains with isolated macropores. The overall morphological variation with the reaction time was explained in terms of the phase separation and the structure freezing by the forced gelation, both of which were induced by the evaporation of methanol during the dipping operation.


Author(s):  
T. M. Correia ◽  
Q. Zhang

Full-perovskite Pb 0.87 Ba 0.1 La 0.02 (Zr 0.6 Sn 0.33 Ti 0.07 )O 3 (PBLZST) thin films were fabricated by a sol–gel method. These revealed both rhombohedral and tetragonal phases, as opposed to the full-tetragonal phase previously reported in ceramics. The fractions of tetragonal and rhombohedral phases are found to be strongly dependent on film thickness. The fraction of tetragonal grains increases with increasing film thickness, as the substrate constraint throughout the film decreases with film thickness. The maximum of the dielectric constant ( ε m ) and the corresponding temperature ( T m ) are thickness-dependent and dictated by the fraction of rhombohedral and tetragonal phase, with ε m reaching a minimum at 400 nm and T m shifting to higher temperature with increasing thickness. With the thickness increase, the breakdown field decreases, but field-induced antiferroelectric–ferroelectric ( E AFE−FE ) and ferroelectric–antiferroelectric ( E FE−AFE ) switch fields increase. The electrocaloric effect increases with increasing film thickness. This article is part of the themed issue ‘Taking the temperature of phase transitions in cool materials’.


1994 ◽  
Vol 346 ◽  
Author(s):  
R. P. S. M. Lobo ◽  
R. L. Moreira ◽  
N. D. S. Mohallem

ABSTRACTBarium titanate ceramics have been obtained by sol-gel methods. The dielectric investigations of these materials revealed the existence of diffuse ferroelectric transitions. By using a phenomenological model, we could demonstrate the existence of a simple relationship between the diffuse character of the transition and the sample grain-size. This effect has been attributed to interactions between charged defects on the grain surfaces and the spontaneous polarization of the material.


2018 ◽  
Vol 233 ◽  
pp. 146-148 ◽  
Author(s):  
R. Peña-Garcia ◽  
Y. Guerra ◽  
B.V.M. Farias ◽  
D. Martínez Buitrago ◽  
A. Franco ◽  
...  

Sign in / Sign up

Export Citation Format

Share Document