Temperature range of the liquid–glass transition
- 作者: Sanditov D.S.1,2, Darmaev M.V.1, Sanditov B.D.1
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隶属关系:
- Buryat State University
- Institute of Physical Materials Science
- 期: 卷 58, 编号 2 (2016)
- 页面: 382-386
- 栏目: Polymers
- URL: https://ogarev-online.ru/1063-7834/article/view/197013
- DOI: https://doi.org/10.1134/S1063783416020256
- ID: 197013
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详细
It has been shown that the currently used method for calculating the temperature range of δTg in the glass transition equation qτg = δTg as the difference δTg = (T12–T13) results in overestimated values, which is explained by the assumption of a constant activation energy of glass transition in deriving the calculation equation (T12 and T13 are the temperatures corresponding to the logarithmic viscosity values of logη = 12 and logη = 13). The methods for the evaluation of δTg using the Williams–Landel–Ferry equation and the model of delocalized atoms are considered, the results of which are in satisfactory agreement with the product qτg (q is the cooling rate of the melt and τg is the structural relaxation time at the glass transition temperature). The calculation of τg for inorganic glasses and amorphous organic polymers is proposed.
作者简介
D. Sanditov
Buryat State University; Institute of Physical Materials Science
编辑信件的主要联系方式.
Email: sanditov@bsu.ru
俄罗斯联邦, ul. Ranzhurova 6a, Ulan-Ude, 670000; ul. Sakhyanovoi 8, Ulan-Ude, 670047
M. Darmaev
Buryat State University
Email: sanditov@bsu.ru
俄罗斯联邦, ul. Ranzhurova 6a, Ulan-Ude, 670000
B. Sanditov
Buryat State University
Email: sanditov@bsu.ru
俄罗斯联邦, ul. Ranzhurova 6a, Ulan-Ude, 670000
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