2022
DOI: 10.1021/acs.macromol.1c02553
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Scaling Theory of Swelling and Deswelling of Polymer Networks

Abstract: We have developed a scaling theory of the elasticity of swollen and deswollen polymer networks. The elasticity of unentangled networks is primarily due to cross-links, and the elasticity of entangled networks is due to trapped entanglements. In preparation conditions, the number of monomers N x in strands of the unentangled network is less than the number of monomers N e0 in an entanglement strand while N x > N e0 for the entangled network. A network weakly entangled at preparation conditions is predicted … Show more

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Cited by 14 publications
(13 citation statements)
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References 32 publications
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“…We take advantage of tetra-PEG gels pioneered by Sakai and colleagues because the network contains a regular structure with fewer defects than common networks and attains elasticity consistent with the phantom network model (Fig. 1A) (25)(26)(27)(28). We show here that a DELSE can, unlike the tetra-PEG gel or common elastomers, achieve ultrahigh SIC.…”
Section: Introductionsupporting
confidence: 52%
“…We take advantage of tetra-PEG gels pioneered by Sakai and colleagues because the network contains a regular structure with fewer defects than common networks and attains elasticity consistent with the phantom network model (Fig. 1A) (25)(26)(27)(28). We show here that a DELSE can, unlike the tetra-PEG gel or common elastomers, achieve ultrahigh SIC.…”
Section: Introductionsupporting
confidence: 52%
“…The elastic free energy density is the elastic energy of each chain , multiplied by the volume density ϕ /( b 3 N e ) of DNA in the network (Rubinstein and Colby, 2003, Yamamoto et al, 2022), Eq. (11) is simplified to by using eq.…”
Section: Methodsmentioning
confidence: 99%
“…The modulus of strongly deswollen slide-ring networks is higher than the modulus of phantom networks because it is dominated by the contribution of fluctuations in the number of monomers between slide-rings, and this contribution increases linearly with the volume fraction as G ≃ k B T ν 0 (ϕ/ϕ 0 ). Note that the predicted concentration dependence of the modulus of deswollen slide-ring gels is even stronger than that of the nonaffine loopy globule model of entangled networks in θ-solvent ( G ≈ ϕ 7/9 ) …”
mentioning
confidence: 88%
“…Note that the predicted concentration dependence of the modulus of deswollen slide-ring gels is even stronger than that of the nonaffine loopy globule model of entangled networks in θsolvent (G ≈ ϕ 7/9 ). 32 We performed multichain bead−spring molecular dynamics simulations that allow spatial fluctuations of rings and compared the simulation results with the predictions of the phantom slide-ring (PSR) model (see section 7 in the Supporting Information). The slide-rings are modeled as seven-membered rings that can freely slide along the bead− spring primary chains.…”
mentioning
confidence: 99%