Effects of the Chain Architecture on the Miscibility of Symmetric Linear/Linear and Star/Star Polymer Blends

2006 ◽  
Vol 39 (12) ◽  
pp. 4235-4239 ◽  
Author(s):  
P. E. Theodorakis ◽  
A. Avgeropoulos ◽  
J. J. Freire ◽  
M. Kosmas ◽  
C. Vlahos
Keyword(s):  
Polymer Blends ◽  
Star Polymer ◽  
Chain Architecture

Thermal, Optical, and Static/Dynamic Mechanical Properties of Linear-core Crosslinked Star Polymer Blends

2011 ◽  
Vol 212 (16) ◽  
pp. 1778-1790 ◽  
Author(s):  
Steven Spoljaric ◽  
Tor Kit Goh ◽  
Anton Blencowe ◽  
Greg G. Qiao ◽  
Robert A. Shanks
Keyword(s):  
Mechanical Properties ◽  
Polymer Blends ◽  
Dynamic Mechanical Properties ◽  
Star Polymer ◽  
Dynamic Mechanical

The Effect of Chain Architecture of In Situ Formed Copolymers on Interfacial Morphology of Reactive Polymer Blends

2005 ◽  
Vol 26 (17) ◽  
pp. 1428-1433 ◽  
Author(s):  
Hwang Yong Kim ◽  
Du Yeol Ryu ◽  
Unyong Jeong ◽  
Dong Han Kho ◽  
Jin Kon Kim
Keyword(s):  
Polymer Blends ◽  
Reactive Polymer ◽  
Interfacial Morphology ◽  
Chain Architecture

Synthesis of Janus POSS star polymer and exploring its compatibilization behavior for PLLA/PCL polymer blends

Polymer ◽  
2018 ◽  
Vol 136 ◽  
pp. 84-91 ◽  
Author(s):  
Di Han ◽  
Tian-jiao Wen ◽  
Ge Han ◽  
Yi-yi Deng ◽  
Yang Deng ◽  
...  
Keyword(s):  
Polymer Blends ◽  
Star Polymer

Theory for conductivity in conducting star polymer blends

2002 ◽  
Vol 126 (2-3) ◽  
pp. 289-293 ◽  
Author(s):  
David T. Wu
Keyword(s):  
Polymer Blends ◽  
Star Polymer

scholarly journals Phase segregation mechanisms of small molecule‐polymer blends unraveled by varying polymer chain architecture

SmartMat ◽  
2021 ◽  
Author(s):  
Jihua Chen ◽  
Sanjib Das ◽  
Ming Shao ◽  
Guoliang Li ◽  
Huada Lian ◽  
...  
Keyword(s):  
Polymer Blends ◽  
Polymer Chain ◽  
Small Molecule ◽  
Phase Segregation ◽  
Chain Architecture

Effective interaction parameter of linear/star polymer blends and comparison with that of linear/linear and star/star blends

2007 ◽  
Vol 126 (17) ◽  
pp. 174904 ◽  
Author(s):  
P. E. Theodorakis ◽  
A. Avgeropoulos ◽  
J. J. Freire ◽  
M. Kosmas ◽  
C. Vlahos
Keyword(s):  
Polymer Blends ◽  
Interaction Parameter ◽  
Effective Interaction ◽  
Star Polymer

Integration of Core-Edge Spectroscopy Methods for the Study of Polymers

1996 ◽  
Vol 54 ◽  
pp. 154-155
Author(s):  
E. G. Rightor
Keyword(s):  
Excited State ◽  
Polymer Blends ◽  
Gas Phase ◽  
Spatial Resolution ◽  
High Spatial Resolution ◽  
Electronic States ◽  
Core Electron ◽  
Bulk Solids ◽  
Development Application

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.

A quantitative image analysis method for the determination of cocontinuity in polymer blends

1993 ◽  
Vol 51 ◽  
pp. 894-895
Author(s):  
William A. Heeschen
Keyword(s):  
Image Analysis ◽  
Polymer Blends ◽  
Quantitative Measurement ◽  
Morphological Evolution ◽  
Phase Ratio ◽  
Irregular Shapes ◽  
Quantitative Image ◽  
Discrete Domains ◽  
A Domains

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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