Interaction of thermal contact resistance and frictional heating in thermoelastic instability |
| |
Affiliation: | 1. CEMEC-PoliBA––Centre of Excellence in Computational Mechanics, V.le Japigia 182, Politecnico di Bari, 70125 Bari, Italy;2. Division of Mechanics, Department of Mechanical Engineering, Linköping University, S–581 83, Linköping, Sweden;3. Department of Mechanical Engineering, University of Michigan, 2250 G.G. Brown Building 2350 Hayward Street, Ann Arbor, MI 48109-2125, USA;1. Hamburg University of Technology, Department of Mechanical Engineering, Am Schwarzenberg-Campus 1, 21073, Hamburg, Germany;2. Imperial College London, Exhibition Road, London, SW7 2AZ, UK;3. Arts et Métiers ParisTech, Department of Mechanical Engineering, 8 Boulevard Louis XIV, 59000 Lille, France;4. Politecnico di BARI, DMMM Dept., V Gentile 182, 70126, Bari, Italy |
| |
Abstract: | Thermoelastic contact problems can posess non-unique and/or unstable steady-state solutions if there is frictional heating or if there is a pressure-dependent thermal contact resistance at the interface. These two effects have been extensively studied in isolation, but their possible interaction has never been investigated. In this paper, we consider an idealized problem in which a thermoelastic rod slides against a rigid plane with both frictional heating and a contact resistance. For sufficiently low sliding speeds, the results are qualitatively similar to those with no sliding. In particular, there is always an odd number of steady-state solutions; if the steady-state is unique it is stable and if it is non-unique, stable and unstable solutions alternate, with the outlying solutions being stable. However, we identify a sliding speed V0 above which the number of steady states is always even (including zero, implying possible non-existence of a steady-state) and again stable and unstable states alternate. A parallel numerical study shows that for V>V0 there are some initial conditions from which the contact pressure grows without limit in time, whereas for V<V0 the system will always tend to one of the stable steady states. |
| |
Keywords: | |
本文献已被 ScienceDirect 等数据库收录! |
|