Abstract
This work elucidates friction in Poly-Ether-Ether-Ketone (PEEK) sliding contacts through multiscale simulations. At the nanoscale, non-reactive classical molecular dynamics (MD) simulations of dry and water-lubricated amorphous PEEK–PEEK interfaces are performed. During a short running-in phase, we observe structural transformations at the sliding interface that result in flattening of the initial nanotopographies accompanied by strong polymer chain alignment in the shearing direction. The MD simulations also reveal a linear pressure – shear stress dependence and large adhesive friction in dry conditions. This dependence, summarized in a nanoscale friction law, is of central importance for our multiscale approach, since it forms a link between MD and elastoplastic contact mechanics calculations. An integration of the nanoscale friction law over the real area of contact yields a macroscopic friction coefficient that allows for a meaningful comparison with measurements from macroscopic tribometer experiments. Severe normal loading conditions result in significant wear and high experimental friction coefficients µ≈0.5–0.7, which are in good agreement with the calculated values from the multiscale approach in dry conditions. For milder experimental loads, our multiscale model suggests that lower friction states with µ≈0.2 originate in the presence of physisorbed molecules (e.g., water), which significantly reduce interfacial adhesion.
Highlights
Nowadays, polymers are increasingly used in tribological applications due to their advantageous properties of low friction, corrosion resistance, biocompatibility, and cost effectiveness
A key element is the real area of contact between rough surfaces [2], which can be extracted from either experiments or contact mechanics calculations [3,4]
For normal forces of 130 mN, 310 mN and 1.05 N, high friction was observed in approximately half of the performed experiments, as the applied load approached the mechanical limit of the thermoplastic
Summary
Polymers are increasingly used in tribological applications due to their advantageous properties of low friction, corrosion resistance, biocompatibility, and cost effectiveness. The shear strength at the contact spots strongly depends on the polymer and counter material and on the presence of moisture, lubricants or transfer layers [9,10,11] at the shearing interface. This makes a direct experimental determination of τ inaccessible for relevant technical surface pairings
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