Combined Duffing nonlinearity and Bliman–Sorine friction dynamics in rubber bearings

The forced harmonic oscillator with combined Duffing cubic stiffness and Bliman–Sorine dynamic friction model is analyzed using Poincaré sections and parameter‑space basins of attraction, constructed as functions of two key oscillator parameters: friction stiffness and forcing amplitude. The analysis uncovers several key dynamical features: (i) chaotic behavior is absent when the cubic stiffness term is weak; (ii) chaotic regimes emerge as soon as the cubic stiffness becomes strong; (iii) the parameter space develops strongly entangled basins, reflecting extreme sensitivity of attractor selection to frictional micro‑mechanics; and (iv) variations in the Bliman–Sorine and Duffing parameters induce pronounced topological changes in basins of attraction. These findings provide new insight into the structure of oscillations in systems governed by the combined Bliman–Sorine and Duffing models. Numerical simulations are performed using a variable‑step Adams–Bashforth–Moulton explicit–implicit scheme to ensure reliable long‑time integration.

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Publication Details

Journal
Mechanics of Advanced Materials and Structures
Published
2026-07-18
DOI
https://doi.org/10.1080/15376494.2026.2702555
Primary Topic
Elasticity and Material Modeling
Type
article
Field-Weighted Citation Impact
0.00

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article

Combined Duffing nonlinearity and Bliman–Sorine friction dynamics in rubber bearings

С. В. Кузнецов
Mechanics of Advanced Materials and Structures
Elasticity and Material Modeling
article

Combined Duffing nonlinearity and Bliman–Sorine friction dynamics in rubber bearings

С. В. Кузнецов
article en

Abstract

The forced harmonic oscillator with combined Duffing cubic stiffness and Bliman–Sorine dynamic friction model is analyzed using Poincaré sections and parameter‑space basins of attraction, constructed as functions of two key oscillator parameters: friction stiffness and forcing amplitude. The analysis uncovers several key dynamical features: (i) chaotic behavior is absent when the cubic stiffness term is weak; (ii) chaotic regimes emerge as soon as the cubic stiffness becomes strong; (iii) the parameter space develops strongly entangled basins, reflecting extreme sensitivity of attractor selection to frictional micro‑mechanics; and (iv) variations in the Bliman–Sorine and Duffing parameters induce pronounced topological changes in basins of attraction. These findings provide new insight into the structure of oscillations in systems governed by the combined Bliman–Sorine and Duffing models. Numerical simulations are performed using a variable‑step Adams–Bashforth–Moulton explicit–implicit scheme to ensure reliable long‑time integration.

Mechanics of Advanced Materials and StructuresVol. 33(1)
Institute for Theoretical and Experimental Physics (RU)
Russian Science Foundation
Openalex Percentile: Top 15%
Elasticity and Material Modeling
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