Kinetic Gelation model predictions of crosslinked polymer network microstructure

1994 ◽  
Vol 49 (14) ◽  
pp. 2207-2217 ◽  
Author(s):  
Kristi S. Anseth ◽  
Christopher N. Bowman
Author(s):  
J. A. N. Zasadzinski ◽  
R. K. Prud'homme

The rheological and mechanical properties of crosslinked polymer gels arise from the structure of the gel network. In turn, the structure of the gel network results from: thermodynamically determined interactions between the polymer chain segments, the interactions of the crosslinking metal ion with the polymer, and the deformation history of the network. Interpretations of mechanical and rheological measurements on polymer gels invariably begin with a conceptual model of,the microstructure of the gel network derived from polymer kinetic theory. In the present work, we use freeze-etch replication TEM to image the polymer network morphology of titanium crosslinked hydroxypropyl guars in an attempt to directly relate macroscopic phenomena with network structure.


Polymer ◽  
2018 ◽  
Vol 153 ◽  
pp. 453-463 ◽  
Author(s):  
M.M. Diaz ◽  
J. Brancart ◽  
G. Van Assche ◽  
B. Van Mele

Soft Matter ◽  
2019 ◽  
Vol 15 (43) ◽  
pp. 8653-8666 ◽  
Author(s):  
Cécile Mussault ◽  
Hui Guo ◽  
Nicolas Sanson ◽  
Dominique Hourdet ◽  
Alba Marcellan

Poly(N-isopropylacrylamide) grafts in a hydrophilic covalently crosslinked polymer network enable efficient T-responsive toughening. Here, we show that graft length is a key-parameter to enhance stiffness and fracture (bulk and adhesion) properties.


2017 ◽  
Vol 9 (1) ◽  
pp. 1-5
Author(s):  
Soojin Lee ◽  
Taewoo Moon ◽  
Kuktae Kwon ◽  
Jin Seuk Kim ◽  
Jungwook Kim ◽  
...  

2012 ◽  
Vol 04 (01) ◽  
pp. 1250007 ◽  
Author(s):  
JUNDIKA CANDRA KURNIA ◽  
ERIK BIRGERSSON ◽  
ARUN S. MUJUMDAR

A phenomenological model for stimuli sensitive hydrogels immersed in water subject to changes in temperature is presented and analyzed. In short, the model takes into account conservation of mass and momentum for polymer network and interstitial fluid with an expression for permeability to capture the rigid skin formation during shrinking. The nature of this expression is secured from the observation of and validation with experimental deformation kinetics. Overall, good agreement is achieved between model predictions and their experimental counterparts; the rigid skin formation and rigid core presence are also captured reasonably well. The model can be extended to account for arbitrary-shaped hydrogels as well as for other types of stimuli-sensitive hydrogels that exhibit rigid-skin formation during shrinking.


2017 ◽  
Vol 5 (4) ◽  
pp. 1533-1540 ◽  
Author(s):  
Seungju Kim ◽  
Xiaocheng Lin ◽  
Ranwen Ou ◽  
Huiyuan Liu ◽  
Xiwang Zhang ◽  
...  

A graphene oxide (GO)–polymer nanocomposite membrane was fabricated by integrating GO nanosheets into a highly crosslinked polymer network on a porous polymer substrate for desalination.


2020 ◽  
Vol 87 (7) ◽  
Author(s):  
Dongjing He ◽  
Yuhang Hu

Abstract A polymeric gel contains a crosslinked polymer network and solvent. Gels can swell or shrink in response to external stimuli. Two typical kinetic processes are involved during the deformation of gels: the viscoelastic and poroelastic responses. Viscoelasticity of gels is generated from local rearrangement of the polymers, while poroelasticity is generated from solvent migration. The coupled time-dependent behaviors of gels can be formulated by coupling a spring-dashpot model with a diffusion–deformation model. Different combinations of spring and dashpot and different ways of dealing with the coupling between solvent migration and rheological models—either through the spring or dashpot—induce significantly different constitutive behaviors and characteristic time-dependent responses of gels. In this work, we quantitatively study how different rheological models coupled with solvent migration affect the transient behavior of gels. We formulate the visco-poroelastic gel theory for the Maxwell model, the Kelvin–Voigt model, and the generalized standard viscoelastic model. In addition, for generalized standard viscoelastic model, we also discuss the different coupling through the secondary spring or the dashpot. The models are implemented into finite element codes, and the transient-state simulations are performed to investigate the time-dependent deformation and frequency-dependent energy dissipation of different rheologically implemented gel models. The result shows that different combinations of spring and dashpot give the gel solid-like properties and liquid-like properties under different time scales; in addition, the coupling of solvent migration with the dashpot in the rheological model results in restrictions of solvent migration under certain length scales.


2012 ◽  
Vol 137 (2) ◽  
pp. 024906 ◽  
Author(s):  
Daming Li ◽  
Thomas Gruhn ◽  
Heike Emmerich

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