Graphene and Graphene Oxide as Nanofiller for Polymer Blends

Author(s):  
Benalia Kouini ◽  
Hossem Belhamdi
2018 ◽  
Vol 156 ◽  
pp. 166-176 ◽  
Author(s):  
Roberto Scaffaro ◽  
Andrea Maio ◽  
Giada Lo Re ◽  
Antonino Parisi ◽  
Alessandro Busacca

ACS Nano ◽  
2011 ◽  
Vol 5 (7) ◽  
pp. 5920-5927 ◽  
Author(s):  
Yewen Cao ◽  
Jing Zhang ◽  
Jiachun Feng ◽  
Peiyi Wu

RSC Advances ◽  
2015 ◽  
Vol 5 (100) ◽  
pp. 82259-82270 ◽  
Author(s):  
Chao-ying Lin ◽  
Ting Liu ◽  
Min Zuo ◽  
Hui-hui Li ◽  
Qi Chen ◽  
...  

The applicability of WLF function to phase separation behavior of filled systems indicates that CRGO hardly changes the viscous diffusion essence of segments. Furthermore, the effect of CRGO on the phase behavior is dependent on their composition.


Author(s):  
E. G. Rightor

Core edge spectroscopy methods are versatile tools for investigating a wide variety of materials. They can be used to probe the electronic states of materials in bulk solids, on surfaces, or in the gas phase. This family of methods involves promoting an inner shell (core) electron to an excited state and recording either the primary excitation or secondary decay of the excited state. The techniques are complimentary and have different strengths and limitations for studying challenging aspects of materials. The need to identify components in polymers or polymer blends at high spatial resolution has driven development, application, and integration of results from several of these methods.


Author(s):  
William A. Heeschen

Two new morphological measurements based on digital image analysis, CoContinuity and CoContinuity Balance, have been developed and implemented for quantitative measurement of morphology in polymer blends. The morphology of polymer blends varies with phase ratio, composition and processing. A typical morphological evolution for increasing phase ratio of polymer A to polymer B starts with discrete domains of A in a matrix of B (A/B < 1), moves through a cocontinuous distribution of A and B (A/B ≈ 1) and finishes with discrete domains of B in a matrix of A (A/B > 1). For low phase ratios, A is often seen as solid convex particles embedded in the continuous B phase. As the ratio increases, A domains begin to evolve into irregular shapes, though still recognizable as separate domains. Further increase in the phase ratio leads to A domains which extend into and surround the B phase while the B phase simultaneously extends into and surrounds the A phase.


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