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@ARTICLE{Sivebaek:12966,
author = {Sivebaek, I.M. and Samoilov, V.N. and Persson, B. N. J.},
title = {{V}elocity {D}ependence of {F}riction of {C}onfined
{H}ydrocarbons},
journal = {Langmuir},
volume = {26},
issn = {0743-7463},
address = {Washington, DC},
publisher = {ACS Publ.},
reportid = {PreJuSER-12966},
pages = {8721 - 8728},
year = {2010},
note = {A part of the present work was carried out in frames of the
European Science Foundation EUROCORES Programme FANAS
supported from the EC Sixth Framework Programme, under
Contract N. ERAS-CT-2003-980409. I.M.S. and V.N.S.
acknowledge support from IFF, FZ-Julich, as well as
hospitality and help of the staff during their research
visits.},
abstract = {We present molecular dynamics friction calculations for
confined hydrocarbon "polymer" solids with molecular lengths
from 20 to 1400 carbon atoms. Two cases are considered: (a)
polymer sliding against a hard substrate and (b) polymer
sliding on polymer. We discuss the velocity dependence of
the frictional shear stress for both cases. In our
simulations, the polymer films are very thin (approximately
3 nm), and the solid walls are connected to a thermostat at
a short distance from the polymer slab. Under these
circumstances we find that frictional heating effects are
not important, and the effective temperature in the polymer
film is always close to the thermostat temperature. In the
first setup (a), for hydrocarbons with molecular lengths
from 60 to 1400 carbon atoms, the shear stresses are nearly
independent of molecular length, but for the shortest
hydrocarbon C(20)H(42) the frictional shear stress is lower.
In all cases the frictional shear stress increases
monotonically with the sliding velocity. For polymer sliding
on polymer (case b) the friction is much larger, and the
velocity dependence is more complex. For hydrocarbons with
molecular lengths from 60 to 140 C atoms, the number of
monolayers of lubricant increases (abruptly) with increasing
sliding velocity (from 6 to 7 layers), leading to a decrease
of the friction. Before and after the layering transition,
the frictional shear stresses are nearly proportional to the
logarithm of sliding velocity. For the longest hydrocarbon
(1400 C atoms) the friction shows no dependence on the
sliding velocity, and for the shortest hydrocarbon (20 C
atoms) the frictional shear stress increases nearly linearly
with the sliding velocity.},
keywords = {Hydrocarbons: chemistry / Polymers: chemistry /
Hydrocarbons (NLM Chemicals) / Polymers (NLM Chemicals) / J
(WoSType)},
cin = {IFF-1},
ddc = {670},
cid = {I:(DE-Juel1)VDB781},
pnm = {Grundlagen für zukünftige Informationstechnologien},
pid = {G:(DE-Juel1)FUEK412},
shelfmark = {Chemistry, Multidisciplinary / Chemistry, Physical /
Materials Science, Multidisciplinary},
typ = {PUB:(DE-HGF)16},
pubmed = {pmid:20210317},
UT = {WOS:000277928100141},
doi = {10.1021/la904476d},
url = {https://juser.fz-juelich.de/record/12966},
}