The forces between layers of poly(ethylene oxide) (PEO), of molecular weigh
ts M = 37 x 10(3) (PEO37) and M = 112 x 10(3) (PEO112) adsorbed onto smooth
, curved solid (mica) surfaces across the good solvent toluene have been de
termined using a surface force balance (SFB). The SFB used is capable of me
asuring both normal interactions F-n(D) as a function of surface separation
D and, with extreme sensitivity, shear or frictional forces F-s(D,nu (s))
between them as they slide past each other at velocity nu (s). The F-n(D) p
rofiles are closely similar to those measured in earlier studies between ad
sorbed PEO layers. The shear or frictional forces between the sliding PEO-b
earing surfaces are very low up to moderate compressions of the adsorbed la
yers (local pressures up to ca. 10(5) N m(-2)), corresponding to effective
friction coefficients mu (eff) = (F-s/F-n) of order 0.003 or less. This is
attributed to the fluid interfacial layer between the adsorbed layers resul
ting from their weak mutual interpenetration. At higher loads F-s increases
markedly, and two forms of behavior are found depending on the PEO molecul
ar weight. For PEO37, a sharp increase in F-s is followed by removal of pol
ymer from within the intersurface gap during sliding, high friction, and ad
hesion between the surfaces. For the longer PEO112, the initial increase in
F-s and in mu (eff) saturates at the highest loads (for the case of mu (ef
f) even decreasing), indicating that the slip plane has moved from the poly
mer/polymer midplane to the polymer/ solid interface. The dependence of F-s
on the sliding velocity in the high-friction regime is weak, suggesting th
at at low compressions there is a thinning of the mutual adsorbed-layer-int
erpenetration region at high nu (s) that offsets the higher viscous dissipa
tion in that region. At the highest loads, when the slip plane has shifted
to the mica surface, the weak F-s(nu (s)) dependence is characteristic of s
liding friction at solid substrates.