% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@ARTICLE{Metri:848278,
author = {Metri, Vishal and Louhichi, Ameur and Yan, Jiajun and
Baeza, Guilhem P. and Matyjaszewski, Krzysztof and
Vlassopoulos, Dimitris and Briels, Willem},
title = {{P}hysical {N}etworks from {M}ultifunctional {T}elechelic
{S}tar {P}olymers: {A} {R}heological {S}tudy by
{E}xperiments and {S}imulations},
journal = {Macromolecules},
volume = {51},
number = {8},
issn = {1520-5835},
address = {Washington, DC},
publisher = {Soc.},
reportid = {FZJ-2018-03539},
pages = {2872 - 2886},
year = {2018},
abstract = {The equilibrium mechanical properties of a cross-linked gel
of telechelic star polymers are studied by rheology and
Brownian dynamics simulations. The Brownian dynamics model
consists of cores to which Rouse arms are attached. Forces
between the cores are obtained from a potential of mean
force model developed by Likos and co-workers. Both
experimentally and in the simulations, networks were created
by attaching sticker groups to the ends of the arms of the
polymers, which were next allowed to form bonds among them
in a one to one fashion. Simulations were sped up by solving
the Rouse dynamics exactly. Moreover, the Rouse model was
extended to allow for different frictions on different
beads. In order to describe the rheology of the
non-cross-linked polymers, it had to be assumed that bead
frictions increase with increasing bead number along the
arms. This friction model could be transferred to describe
the rheology of the network without any adjustments other
than an overall increase of the frictions due to the
formation of bonds. The slowing down at intermediate times
of the network rheology compared to that of the
non-cross-linked polymers is well described by the model.
The percentage of stickers involved in forming inter-star
bonds in the system was determined to be $25\%,$ both from
simulations and from an application of the Green–Tobolsky
relation to the experimental plateau value of the shear
relaxation modulus. Simulations with increasing cross-link
percentages revealed that on approaching the gel transition
the shear relaxation modulus develops an algebraic tail,
which gets frozen at a percentage of maximum cross-linking
of about $11\%.$},
cin = {ICS-3},
ddc = {540},
cid = {I:(DE-Juel1)ICS-3-20110106},
pnm = {551 - Functional Macromolecules and Complexes (POF3-551)},
pid = {G:(DE-HGF)POF3-551},
typ = {PUB:(DE-HGF)16},
pubmed = {pmid:29910512},
UT = {WOS:000431088700012},
doi = {10.1021/acs.macromol.7b02613},
url = {https://juser.fz-juelich.de/record/848278},
}