Evaluation of the relaxation time for the amorphous styrene oligomer PSA-500 obtained from various measurement methods near the glass-transition temperature

2019 ◽  
Vol 672 ◽  
pp. 101-106
Author(s):  
Jun Fujimura ◽  
Minato Sugisaki ◽  
Eri Nishiyama ◽  
Masanobu Takatsuka ◽  
Kaito Sasaki ◽  
...  
2020 ◽  
Vol 62 (10) ◽  
pp. 1706
Author(s):  
Д.С. Сандитов ◽  
В.В. Мантатов ◽  
С.Ш. Сангадиев

Using the model of delocalized atoms, a substantiation and generalization of the Schmelzer glass transition criterion is proposed. In contrast to the Bartenev and Volkenstein - Ptitsyn approaches, in the generalized kinetic glass transition criterion, along with the relaxation time and the cooling rate of the melt, the glass transition temperature and an almost universal dimensionless constant appear, which is determined by the fraction of the fluctuation volume frozen at the glass transition temperature. The idea is developed that the liquid goes into a glassy state when its cooling rate q reaches a certain fraction of C_g of the characteristic cooling rate q_g=(T_g/taug), which is closely related to the relaxation time of the structure tau_g at the glass transition temperature T_g.


Soft Matter ◽  
2021 ◽  
Author(s):  
Bhaskar Soman ◽  
Christopher M. Evans

Dynamic networks with precise spacers between boronic ester bonds were investigated over a broad temperature window. Arrhenius behavior breaks down and an increase in relaxation time is observed when approach the glass transition temperature.


2017 ◽  
Vol 19 (40) ◽  
pp. 27442-27451 ◽  
Author(s):  
Yao Fu ◽  
Vera Bocharova ◽  
Mengze Ma ◽  
Alexei P. Sokolov ◽  
Bobby G. Sumpter ◽  
...  

Backbone rigidity, counterion size and the static dielectric constant affect the glass transition temperature, segmental relaxation time and decoupling between counterion and segmental dynamics in significant manners.


1977 ◽  
Vol 55 (13) ◽  
pp. 2517-2522 ◽  
Author(s):  
D. Ceccaldi

A general kinetic theory is used to explain the shapes of photoionized sample luminescence curves perturbed by thermal jumps (Δ ∼ 1 K, rise time ∼ 1 s). The samples studied are photoactivated organic vitreous solutions of TMPD/MCH 10−3 M and TMPD/3-MP 10−3 M. The experiments are performed within a temperature range (63–91 K) which includes the glass transition temperature Tg. It is shown that there is a slow diffusion of the trapped electrons towards the cation and competition between thermal detrapping and tunneling. The tunneling/thermal detrapping ratio Y is not time dependent during an isothermal luminescence and is only slowly temperature dependent if T ≤ Ty. Ty is very close to Tg. For T > Ty, Y decreases rapidly with T. The activation energy for thermal detrapping shows a maximum when the temperature reaches [Formula: see text] The glass transition temperature Tg may therefore be defined empirically as:[Formula: see text]Finally we obtain a glassy matrix relaxation time, τ, which decreases with T.


1991 ◽  
Vol 244 ◽  
Author(s):  
John W. Shea ◽  
John M. Turnipseed ◽  
Carl R. Taylor ◽  
James R. Petisce ◽  
Bob J. Overton

ABSTRACTThis paper describes four key measurements of critical coating performance attributes which can affect coated optical fiber performance. The four measurement methods to be described are: 1) primary coating adhesion, 2) coating toughness, 3) primary coating equilibrium modulus, and 4) primary coating glass transition temperature.


2007 ◽  
Vol 258 (1) ◽  
pp. 152-161 ◽  
Author(s):  
Jean Marc Saiter ◽  
Jean Grenet ◽  
Eric Dargent ◽  
Allisson Saiter ◽  
Laurent Delbreilh

2014 ◽  
Vol 341 (1) ◽  
pp. 45-50 ◽  
Author(s):  
Hadj Bahous ◽  
Manil M. Soufi ◽  
Laurent Meuret ◽  
Mohammed Benzohra

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