2019
DOI: 10.1039/c9sm00292h
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Tendomers – force sensitive bis-rotaxanes with jump-like deformation behavior

Abstract: Tendomers (pairs of rotaxanes connected at the first slide ring) display a jump-like strain softening under an applied external force with a switching point that is set by the slide ring density.

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Cited by 15 publications
(34 citation statements)
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“…For our study, we use the Bond Fluctuation Model (BFM) 47,48 , which is a well known lattice based Monte-Carlo method that has been used frequently to simulate polymer model systems [49][50][51] , solutions 52,53 , membranes 54 , melts 55,56 , or networks 57,58 . In this simulation method, chains are represented by a connected set of small cubes that resemble the monomers of the chain.…”
Section: Computer Simulationsmentioning
confidence: 99%
“…For our study, we use the Bond Fluctuation Model (BFM) 47,48 , which is a well known lattice based Monte-Carlo method that has been used frequently to simulate polymer model systems [49][50][51] , solutions 52,53 , membranes 54 , melts 55,56 , or networks 57,58 . In this simulation method, chains are represented by a connected set of small cubes that resemble the monomers of the chain.…”
Section: Computer Simulationsmentioning
confidence: 99%
“…It is therefore necessary to construct a novel theory to explain the low Young’s moduli of SR gels that considers the slidability of the cross-linking points. Several studies have aimed to reveal the origin of the elasticity of SR gels. Ito proposed a three-chain model in which chain segments can move through a free junction between the three chains . For uniaxial deformation, the free junction model gives a Young’s modulus of zero, which is inconsistent with the finite Young’s moduli of the SR gels measured by tensile experiments.…”
mentioning
confidence: 99%
“…In spite of being a non-specific model of polymer dynamics, the BFM was successfully used to study a large variety of physical effects in two-and three dimensions like, e.g., static [18][19][20][21][22][23][24][25][26][27][28][29] and dynamic [18,[30][31][32][33] properties of linear chains, polymer rings [27,34], polymer blends and interfaces [35,36], gels and networks [37], glass transition [38][39][40], polymer blends [41], (co)polymers at surfaces [42], polymer brushes in good solvents [43][44][45][46][47][48][49], polymer thin films [50][51][52], equilibrium polymers [29,53,54], general self-assembly [55][56][57], networks and gel point [58][59][60][61], olympic gels…”
Section: Monte Carlo Simulations Of Polymer Systemsmentioning
confidence: 99%