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By Dieter Besdo, Bodo Heimann, Manfred Klüppel, Matthias Kröger, Peter Wriggers, Udo Nackenhorst

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Extra info for Elastomere Friction: Theory, Experiment and Simulation (Lecture Notes in Applied and Computational Mechanics, Volume 51)

Example text

Meier, and M. Kl¨ uppel Fig. 7 Uniaxial multihysteresis measurement and fit, inset shows parameter set, T = 22◦ C, SB6R2. The set of fitted parameters is given as an inset. Some parameters can be assumed to have specified values. These parameters are recognizable from the fitting error = 0 in the right column. The parameter sset,0 can be calculated from the evaluated set stresses and the glass transition temperature Tg of the rubber. 5 calculated by Einstein for delude rigid spheres. 6 MPa for SBR, but only under the assumption that there are no filler-induced entanglements.

Polym. Sci. 164, 1–86 (2003) 8. : Hyperelasticity and stress softening of filler reinforced polymer networks. In: Macromol. , vol. 200, pp. 31–43 (2003) 52 H. Lorenz, J. Meier, and M. Kl¨ uppel 9. : Impact of pre-strain on dynamicmechanical properties of carbon black and silica filled rubbers. ) Constitutive Models for Rubber III, p. 333. Swets & Zeitlinger, Lisse (2003) 10. : Modelling of stress softening and filler induced hysteresis of elastomer materials. ) Constitutive Models for Rubber IV, p.

A second characteristic effect caused by fillers is the pronounced hysteresis which is related to the dissipation of mechanical energy. All these effects are temperature- and time-dependent and are interrelated due to their common origin, but neither the elastomer nor the powderous filler alone shows such behaviour. The filler is composed of relatively stiff particles that do not undergo significant deformation by themselves. Also, the entropy-elastic behaviour of the elastomer or rubber matrix is quite well understood [3–6].

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