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@ARTICLE{Miyashita:1015193,
author = {Miyashita, N. and Yakini, A. E. and Pyckhout-Hintzen, W.
and Persson, Bo},
title = {{S}liding friction on ice},
journal = {The journal of chemical physics},
volume = {158},
number = {17},
issn = {0021-9606},
address = {Melville, NY},
publisher = {American Institute of Physics},
reportid = {FZJ-2023-03589},
pages = {174702},
year = {2023},
abstract = {We study the friction when rectangular blocks made from
rubber, polyethylene, and silica glass are sliding on ice
surfaces at different temperatures ranging from -40 to 0
°C, and sliding speeds ranging from 3 μm/s to 1 cm s-1. We
consider a winter tire rubber compound both in the form of a
compact block and as a foam with $∼10\%$ void volume. We
find that both rubber compounds exhibit a similar friction
on ice for all studied temperatures. As in a previous study
at low temperatures and low sliding speeds, we propose that
an important contribution to the friction force is due to
slip between the ice surface and ice fragments attached to
the rubber surface. At temperatures around 0 °C (or for
high enough sliding speeds), a thin pre-melted water film
will occur at the rubber-ice interface, and the contribution
to the friction from shearing the area of real contact is
small. In this case, the dominant contribution to the
friction force is due to viscoelastic deformations of the
rubber by the ice asperities. The sliding friction for
polyethylene (PE) and silica glass (SG) blocks on ice
differs strongly from that of rubber. The friction
coefficient for PE is ∼0.04-0.15 and is relatively weakly
velocity dependent except close to the ice melting
temperature where the friction coefficient increases toward
low sliding speeds. Silica glass exhibits a similarly low
friction as PE for T > -10 °C but very large friction
coefficients (of order unity) at low temperatures. For both
PE and SG, unless the ice track is very smooth, the friction
force depends on the position x along the sliding track.
This is due to bumps on the ice surface, which are sheared
off by the elastically stiff PE and SG blocks, resulting in
a plowing-type of contribution to the friction force. This
results in friction coefficients, which locally can be very
large ∼1, and visual inspection of the ice surface after
the sliding acts show ice wear particles (white powder) in
regions where ice bumps occur. Similar effects can be
expected for rubber blocks below the rubber glass transition
temperature, and the rubber is in the (elastically stiff)
glassy state.},
cin = {PGI-1 / IAS-1 / IBI-8 / JCNS-1},
ddc = {530},
cid = {I:(DE-Juel1)PGI-1-20110106 / I:(DE-Juel1)IAS-1-20090406 /
I:(DE-Juel1)IBI-8-20200312 / I:(DE-Juel1)JCNS-1-20110106},
pnm = {5211 - Topological Matter (POF4-521)},
pid = {G:(DE-HGF)POF4-5211},
typ = {PUB:(DE-HGF)16},
pubmed = {37125718},
UT = {WOS:001010685000009},
doi = {10.1063/5.0147524},
url = {https://juser.fz-juelich.de/record/1015193},
}