The forces between layers of poly(ethylene oxide) (PEO), of molecular weights M = 37 × 10 3 (PEO37) and M = 112 × 10 3 (PEO112) adsorbed onto smooth, curved solid (mica) surfaces across the good solvent toluene have been determined using a surface force balance (SFB). The SFB used is capable of measuring both normal interactions F n ( D ) as a function of surface separation D and, with extreme sensitivity, shear or frictional forces F s ( D, v s ) between them as they slide past each other at velocity v s . The F n ( D ) profiles are closely similar to those measured in earlier studies between adsorbed PEO layers. The shear or frictional forces between the sliding PEO-bearing surfaces are very low up to moderate compressions of the adsorbed layers (local pressures up to ca. 10 5 N m -2 ), corresponding to effective friction coefficients μ eff = ( F s / F n ) of order 0.003 or less. This is attributed to the fluid interfacial layer between the adsorbed layers resulting from their weak mutual interpenetration. At higher loads F s increases markedly, and two forms of behavior are found depending on the PEO molecular weight. For PEO37, a sharp increase in F s is followed by removal of polymer from within the intersurface gap during sliding, high friction, and adhesion between the surfaces. For the longer PEO112, the initial increase in F s and in μ eff saturates at the highest loads (for the case of μ eff even decreasing), indicating that the slip plane has moved from the polymer/polymer midplane to the polymer/solid interface. The dependence of F s on the sliding velocity in the high-friction regime is weak, suggesting that at low compressions there is a thinning of the mutual adsorbed-layer-interpenetration region at high v s that offsets the higher viscous dissipation in that region. At the highest loads, when the slip plane has shifted to the mica surface, the weak F s ( v s ) dependence is characteristic of sliding friction at solid substrates.
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Raviv et al. (2001) studied this question.
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