Dielectric Study on the Heterogeneous Dynamics of Miscible Polyisoprene/Poly(vinyl ethylene) Blends:  Estimation of the Relevant Length Scales for the Segmental Relaxation Dynamics

2003 ◽  
Vol 36 (10) ◽  
pp. 3699-3708 ◽  
Author(s):  
Yuji Hirose ◽  
Osamu Urakawa ◽  
Keiichiro Adachi
2016 ◽  
Vol 18 (29) ◽  
pp. 19955-19965 ◽  
Author(s):  
Tapabrata Dam ◽  
Sidhartha S. Jena ◽  
Dillip K. Pradhan

An insight into thermally activated ion-hopping, relaxation dynamics and the coupled ion-conduction mechanism observed in ion-conducting polymer clay composites.


2009 ◽  
Vol 131 (34) ◽  
pp. 12201-12210 ◽  
Author(s):  
Els Braeken ◽  
Gert De Cremer ◽  
Philippe Marsal ◽  
Gérard Pèpe ◽  
Klaus Müllen ◽  
...  

Soft Matter ◽  
2019 ◽  
Author(s):  
Manisha Handa ◽  
Parbati Biswas

The segmental relaxation dynamics of ring polymers in dilute solutions ranges from the fast local motions at short times, decelerated due to HI to the global motions at long times, enhanced due to HI, irrespective of the size.


2017 ◽  
Vol 51 (1) ◽  
pp. 195-203 ◽  
Author(s):  
Weizhao Ren ◽  
Yuping Wang ◽  
Xin Chen ◽  
Biao Zuo ◽  
Xianjing Zhou ◽  
...  

2020 ◽  
Vol 153 (23) ◽  
pp. 234502
Author(s):  
Swarup Banerjee ◽  
Pradip Kr. Ghorai ◽  
Suman Das ◽  
Juriti Rajbangshi ◽  
Ranjit Biswas

Polymers ◽  
2019 ◽  
Vol 11 (6) ◽  
pp. 979 ◽  
Author(s):  
Na Wang ◽  
Xuebang Wu ◽  
C.S. Liu

The segmental relaxation dynamics of poly(methyl methacrylate)/silica (PMMA/SiO2) nanocomposites with different compositions ( ϕ SiO 2 ) near and above the glass transition temperature were investigated by mechanical spectroscopy. At ϕ SiO 2 ≤ 0.5%, the α peak temperature hardly changes with ϕ SiO 2 , but that of α’ relaxation composed of Rouse and sub-Rouse modes decreases by 15 °C due to the increase of free volume. At ϕ SiO 2 ≥ 0.7%, both α and α’ relaxations shift to high temperatures because of the steric hindrance introduced by nanoparticle agglomeration. On the other hand, with increasing ϕ SiO 2 , the peak height for α relaxation increases at ϕ SiO 2 ≤ 0.5% and then decreases at ϕ SiO 2 ≥ 0.7%, but that for α’ relaxation shows an opposite behavior. This is because at low ϕ SiO 2 , the short-chain segments related to α relaxation can easily bypass the particles, but the longer-chain segments related to α’ relaxation cannot. At high ϕ SiO 2 , the polymer chains were bound to the nanoparticles due to the physical adsorption effect, leading to the decrease of relaxation unit concentration involved in α relaxation. However, the dissociation of those bonds with heating and the concentration heterogeneity of polymer chains result in the increase of peak height for α’ relaxation.


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