Friction of poroelastic contacts with thin hydrogel films

TL;DR

This study investigates how thin hydrogel films' frictional behavior depends on sliding velocity and water drainage, revealing a critical Péclet number that influences contact shape and friction force, supported by experimental and poroelastic modeling.

Contribution

It introduces a novel optical setup to image contact shape during sliding and links contact behavior to a Péclet number, advancing understanding of poroelastic hydrogel friction.

Findings

Friction force peaks at Pe≈1.

Contact area decreases when Pe>1.

Contact shape becomes asymmetric at higher velocities.

Abstract

We report on the frictional behaviour of thin poly(dimethylacrylamide) (PDMA) hydrogels films grafted on glass substrates in sliding contact with a glass spherical probe. Friction experiments are carried out at various velocities and applied normal loads with the contact fully immersed in water. In addition to friction force measurements, a novel optical set-up is designed to image the shape of the contact under steady-state sliding. The velocity-dependence of both friction force $F_t$ and contact shape is found to be controlled by a P\'eclet number Pe defined as the ratio of the time $\tau$ needed to drain the water out of the contact region to a contact time $a/v$, where $v$ is the sliding velocity and $a$ is the contact radius. When Pe<1, the equilibrium circular contact achieved under static normal indentation remains unchanged during sliding. Conversely, for Pe>1, a decrease in the contact area is observed together with the development of a contact asymmetry when the sliding velocity is increased. A maximum in $F_t$ is also observed at Pe~$\approx$~1. These experimental observations are discussed in the light of a poroelastic contact model based on a thin film approximation. This model indicates that the observed changes in contact geometry are due to the development of a pore pressure imbalance when Pe>1. An order of magnitude estimate of the friction force and its dependence on normal load and velocity is also provided under the assumption that most of the frictional energy is dissipated by poroelastic flow at the leading and trailing edges of the sliding contact.