Theoretical Equilibrium Moduli and Swelling Extents for Elastomers Crosslinked in Solution

1990 ◽  
Vol 63 (1) ◽  
pp. 46-55 ◽  
Author(s):  
J. P. Queslel ◽  
J. E. Mark

Abstract Equilibrium elongation moduli and swelling properties have been calculated for amorphous polymer networks prepared in a diluted reference state of polymer volume fraction υ2C. The three molecular elasticity theories employed are based on (i) an idealized affine deformation model (in which the constraints on junction fluctuations are infinite), (ii) an idealized phantom chain model (in which the constraints are absent), and (iii) the more realistic Flory-Erman theory (in which the constraints vary with crosslinking conditions, degree of swelling, and extent of elongation). A discussion of the dependence of the constraint parameter κ on υ2C is given, and is applied to the calculation of stress-strain isotherms in elongation specifically for cis-polyisoprene cured with dicumyl peroxide. The experimental dependence of κ on υ2C investigated by Erman and Mark was found to be similar to the dependence of the plateau modulus on dilution, and this is consistent with the constrained contour model proposed by Erman and Monnerie.

Polymers ◽  
2020 ◽  
Vol 12 (4) ◽  
pp. 767 ◽  
Author(s):  
Sergey Panyukov

A review of the main elasticity models of flexible polymer networks is presented. Classical models of phantom networks suggest that the networks have a tree-like structure. The conformations of their strands are described by the model of a combined chain, which consists of the network strand and two virtual chains attached to its ends. The distribution of lengths of virtual chains in real polydisperse networks is calculated using the results of the presented replica model of polymer networks. This model describes actual networks having strongly overlapping and interconnected loops of finite sizes. The conformations of their strands are characterized by the generalized combined chain model. The model of a sliding tube is represented, which describes the general anisotropic deformations of an entangled network in the melt. I propose a generalization of this model to describe the crossover between the entangled and phantom regimes of a swollen network. The obtained dependence of the Mooney-Rivlin parameters C 1 and C 2 on the polymer volume fraction is in agreement with experiments. The main results of the theory of heterogeneities in polymer networks are also discussed.


1989 ◽  
Vol 62 (5) ◽  
pp. 800-819 ◽  
Author(s):  
J. P. Queslel

Abstract Characterization of randomly crosslinked networks requires a topological description of imperfect network structure and a molecular-elasticity theory, preferably with a minimum number of adjustable parameters, relating macroscopic stress and strain or swelling ratios to molecular deformation. It is shown that simple relationships exist between the molecular weight between consecutive junctions, the molecular weight of linear precursor chains, the cycle rank, and the number of junctions for networks having no defects other than chain ends. The idealized affine deformation model (in which the constraints on junction fluctuations are infinite) and the idealized phantom-chain model (in which the constraints are absent) are inadequate for network characterization. The more realistic Flory-Erman constrained junction model is applied to the description of cis-polyisoprene cured with dicumyl peroxide. Swelling equilibrium experiments are in agreement with stress-strain measurements. Analysis of these stress-strain data with the constrained-junction and constrained-chain models gives similar results. This validates the Flory hypothesis that it is generally sufficient to concentrate the effects of the constraints on the junctions. Nevertheless, the constrained chain model proposed by Erman and Monnerie has the advantage of depending on one parameter, KG, instead of two, κ and ζ, for the constrained junction model.


1992 ◽  
pp. 79-98
Author(s):  
Ferenc Horkay ◽  
Erik Geissler ◽  
Anne-Marie Hecht ◽  
Miklos Zrinyi

Langmuir ◽  
2020 ◽  
Vol 36 (42) ◽  
pp. 12460-12472 ◽  
Author(s):  
Edwin C. Johnson ◽  
Joshua D. Willott ◽  
Isaac J. Gresham ◽  
Timothy J. Murdoch ◽  
Ben A. Humphreys ◽  
...  

2010 ◽  
Vol 119 (6) ◽  
pp. 3531-3537 ◽  
Author(s):  
D. E. Rodríguez-Félix ◽  
M. M. Castillo-Ortega ◽  
D. Real-Félix ◽  
J. Romero-García ◽  
A. S. Ledezma-Pérez ◽  
...  

Polymer ◽  
2006 ◽  
Vol 47 (17) ◽  
pp. 6226-6235 ◽  
Author(s):  
Seong Hyun Yoo ◽  
Claude Cohen ◽  
Chung-Yuen Hui

e-Polymers ◽  
2007 ◽  
Vol 7 (1) ◽  
Author(s):  
Gul Bali Shah

AbstractThe effect of bimodality i.e. blending short and long chain (0 to 80 % w/w) silicone prepolymers, and that of concentration of the crosslinker on the tensile properties such as percent elongation at break (%Eb), ultimate tensile strength (UTS), 100 % modulus and elastic modulus (E) has been investigated. It was found out that the greater amount of crosslinker used for crosslinking provide an additional reinforcement to the silicone network whereas bimodality further significantly accentuates this effect. Remarkably, the %Eb of the silicone networks was found to increase to an average of 2.4 times than that of the monomodal network, cured in each of the three series of bimodal networks cured with 3.9, 9.1 and 12.3% of crosslinker. The optimum property in each case was observed at about 70 mol % of P100. The over all order of sensitivity of these properties up to about 70 mol % of short chain prepolymer has been observed to be as: %Eb > UTS > 100% modulus > elastic modulus. It has been shown that in addition to the previously published reports the tensile properties are acutely dependent not only upon the degree of crosslinking and primary molecular weight; but also on bimodality and crosslinker concentration for preparation of the unfilled silicone polymer networks. The concept of phase inversion (or phase transition) associated with the optimum properties in polymer blends has for the first time been applied to the bimodal polymer networks. It has been observed that the maxima in tensile properties generally corresponds to phase inversion which takes place at 0.5 volume fraction (70 mol %) of short chain (P100) prepolymer which is in accordance with the literature for other systems.


Polymers ◽  
2020 ◽  
Vol 12 (11) ◽  
pp. 2476 ◽  
Author(s):  
Sabina Horodecka ◽  
Adam Strachota ◽  
Beata Mossety-Leszczak ◽  
Beata Strachota ◽  
Miroslav Šlouf ◽  
...  

Physically crosslinked low-temperature elastomers were prepared based on linear polydimethylsiloxane (PDMS) elastic chains terminated on both ends with mesogenic building blocks (LC) of azobenzene type. They are generally (and also structurally) highly different from the well-studied LC polymer networks (light-sensitive actuators). The LC units also make up only a small volume fraction in our materials and they do not generate elastic energy upon irradiation, but they act as physical crosslinkers with thermotropic properties. Our elastomers lack permanent chemical crosslinks—their structure is fully linear. The aggregation of the relatively rare, small, and spatially separated terminal LC units nevertheless proved to be a considerably strong crosslinking mechanism. The most attractive product displays a rubber plateau extending over 100 °C, melts near 8 °C, and is soluble in organic solvents. The self-assembly (via LC aggregation) of the copolymer molecules leads to a distinctly lamellar structure indicated by X-ray diffraction (XRD). This structure persists also in melt (polarized light microscopy, XRD), where 1–2 thermotropic transitions occur. The interesting effects of the properties of this lamellar structure on viscoelastic and rheological properties in the rubbery and in the melt state are discussed in a follow-up paper (“Part II”). The copolymers might be of interest as passive smart materials, especially as temperature-controlled elastic/viscoelastic mechanical coupling. Our study focuses on the comparison of physical properties and structure–property relationships in three systems with elastic PDMS segments of different length (8.6, 16.3, and 64.4 repeat units).


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