- Open Access
Viscoelastic toy model explaining the static friction paradox in stick-slip instability without friction laws
Phys. Rev. E 111, 065504 – Published 18 June, 2025
DOI: https://doi.org/10.1103/dn4g-chy7
Abstract
The relaxation oscillation in sliding systems is termed stick-slip (SS) since the two surfaces in contact seem to repeat the stick and slip states. However, several precise measurements have revealed that extremely slow slip occurs in even apparently stick states before every stick-to-slip transition, which is here termed the static friction paradox. This study theoretically investigates instabilities induced by solid viscoelasticity using a minimal toy model without friction laws: a two-degrees-of-freedom sliding system consisting of a rigid probe and a Kelvin-Voigt viscoelastic foundation (VEF). Taking advantage of its simplicity, we discuss the mechanisms generating various system dynamics based on stability analysis and numerical simulation. As a result, surprisingly, even though the sliding system does not employ static friction, it exhibits intermittent oscillation resembling the typical SS instability. It comprises two slip states for the contact between the probe and the VEF, i.e., slow-slip and fast-slip states, providing a purely mechanical explanation for the static friction paradox.
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- See Supplemental Material at http://link.aps.org/supplemental/10.1103/dn4g-chy7 for the animations of the numerical results. The supplemental files are movies that visualize the numerical results. Movies S1 to S4 are for Figs. 3– 3, and Movies S4 and S5 are for Fig. 6. The moving open circle (black) and the stationary solid circle (blue) are the probe tip position and the equilibrium point, respectively. The symbols , , and in the movies represent the dimensionless position , the dimensionless position , and the dimensionless relative displacement , respectively.
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