Matrix-Mediated Crystallization of Explosive Materials in Crosslinked Polymer Network

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

Polymers ◽  
2018 ◽  
Vol 10 (10) ◽  
pp. 1156 ◽  
Author(s):  
Grigorios Megariotis ◽  
Georgios Vogiatzis ◽  
Aristotelis Sgouros ◽  
Doros Theodorou

In previous work by the authors, a new methodology was developed for Brownian dynamics/kinetic Monte Carlo (BD/kMC) simulations of polymer melts. In this study, this methodology is extended for dynamical simulations of crosslinked polymer networks in a coarse-grained representation, wherein chains are modeled as sequences of beads, each bead encompassing a few Kuhn segments. In addition, the C++ code embodying these simulations, entitled Engine for Mesoscopic Simulations for Polymer Networks (EMSIPON) is described in detail. A crosslinked network of cis-1,4-polyisoprene is chosen as a test system. From the thermodynamic point of view, the system is fully described by a Helmholtz energy consisting of three explicit contributions: entropic springs, slip springs and non-bonded interactions. Entanglements between subchains in the network are represented by slip springs. The ends of the slip springs undergo thermally activated hops between adjacent beads along the chain backbones, which are tracked by kinetic Monte Carlo simulation. In addition, creation/destruction processes are included for the slip springs at dangling subchain ends. The Helmholtz energy of non-bonded interactions is derived from the Sanchez–Lacombe equation of state. The isothermal compressibility of the polymer network is predicted from equilibrium density fluctuations in very good agreement with the underlying equation of state and with experiment. Moreover, the methodology and the corresponding C++ code are applied to simulate elongational deformations of polymer rubbers. The shear stress relaxation modulus is predicted from equilibrium simulations of several microseconds of physical time in the undeformed state, as well as from stress-strain curves of the crosslinked polymer networks under deformation.


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