4.6 Article

Viscoelastic dissipation in repeated normal indentation of an Hertzian profile

期刊

出版社

PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.ijsolstr.2021.111362

关键词

Viscoelasticity; Dissipation; Hertzian profile; Contact mechanics

资金

  1. Italian Ministry of Education, University and Research (MIUR) under the program Departments of Excellence'' [L.232/2016]
  2. ON Ricerca e Innovazione 2014-2020-Azione I.2 [407, AIM1895471]
  3. Regione Puglia (Italy), project ENOVIM within the call Progetti di ricerca scientifica innovativi di elevato standard internazionale [CUP: D95F21000910002, 89, 25]

向作者/读者索取更多资源

The study indicates that simple exact solutions exist for the indentation problem in a viscoelastic halfspace, but only apply when the contact area is increasing; in cyclic repeated indentation with pulsating loads, more energy is dissipated during the first indentation cycle compared to subsequent ones. In load controlled systems, maximum dissipation occurs at an angular frequency close to the reciprocal of material relaxation time, but in displacement controlled systems, dissipation is much lower.
Simple exact solutions are known for the indentation problem of a viscoelastic halfspace by a rigid sphere only as long as the contact area is growing. We consider instead a more general cyclic repeated indentation with a pulsating load with a period of zero load. We show that a combination of exact with empirical relaxation solutions coming from simple uniaxial cases is sufficiently accurate to estimate the energy dissipated per cycle, which we report for the standard 3-elements solid and periodic half-sine loading for various parameters. The theoretical predictions favourably compare with boundary element numerical simulations. We find more energy is dissipated during the first indentation cycle with respect to the subsequent ones, due to the residual indentation left in the viscoelastic half-space. In load controlled systems, the maximum dissipation is reached at an angular frequency that is close to the reciprocal of the relaxation time of the material both for the first and subsequent cycles, but this is in general not true when displacement controlled systems are considered, when dissipation is much lower for subsequent cycles.

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