2011
DOI: 10.1021/ma201386t
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Strain Hardening and Strain Softening of Reversibly Cross-Linked Supramolecular Polymer Networks

Abstract: The large amplitude oscillatory shear behavior of metallo-supramolecular polymer networks formed by adding bis-Pd(II) cross-linkers to poly(4-vinylpyridine) (PVP) in dimethyl sulfoxide (DMSO) solution is reported. The influence of scanning frequency, dissociation rate of cross-linkers, concentration of cross-linkers, and concentration of PVP solution on the large amplitude oscillatory shear behavior is explored. In semidilute unentangled PVP solutions, above a critical scanning frequency, strain hardening of b… Show more

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Cited by 60 publications
(73 citation statements)
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“…Purely synthetic materials have been designed with covalent networks strengthened by non‐covalent interactions, such as hydrophobic bonds49, 50 and hydrogen bonding,51–53 in an analogous way to achieve unique physical properties. Metal coordination interactions appear to have this function also, as illustrated here and by others 30, 54…”
Section: Mimicking the Ph Increase Of Byssal Processingsupporting
confidence: 73%
“…Purely synthetic materials have been designed with covalent networks strengthened by non‐covalent interactions, such as hydrophobic bonds49, 50 and hydrogen bonding,51–53 in an analogous way to achieve unique physical properties. Metal coordination interactions appear to have this function also, as illustrated here and by others 30, 54…”
Section: Mimicking the Ph Increase Of Byssal Processingsupporting
confidence: 73%
“…The nonlinear strain sweep results are similar to the nonlinear steady shear results shown in Figure 6, and although we do not pursue it further here, we therefore infer that the strain hardening is also caused by nonlinear high tension along stretched polymer chains. 31 …”
Section: Resultsmentioning
confidence: 99%
“…When rescaling the differential modulus K by the low frequency elastic modulus G 0 and the stress measured by σ c , we can directly compare the non-linear response of gels at different volume fractions, independently of their different stiffness in the linear response regime. Fig.3 (a) shows how, for relatively small volume fraction (φ = 5% and φ = 7.5%), the gels exhibit a linear elastic response at small deformations (the initial flat part of K/G 0 as a function of σ/σ c ), followed by a pronounced softening before entering a strain-hardening regime at larger deformations [13,14,49,50]. The strain hardening is characterized by a power law scaling K/G 0 ∼ (σ/σ c ) α , similar to the one found in semiflexible polymer networks [51,52] with an exponent α = 3/2, at φ = 0.05, 0.075.…”
Section: Softening and Hardeningmentioning
confidence: 99%