scholarly journals Frictional heating on faults: Stable sliding versus stick slip

1998 ◽  
Vol 103 (B4) ◽  
pp. 7413-7420 ◽  
Author(s):  
Stephen R. Brown
2006 ◽  
Vol 128 (4) ◽  
pp. 681-696 ◽  
Author(s):  
P. Samyn ◽  
W. Van Paepegem ◽  
J. S. Leendertz ◽  
A. Gerber ◽  
L. Van Schepdael ◽  
...  

Polymer composites are increasingly used as sliding materials for high-loaded bearings, however, their tribological characteristics are most commonly determined from small-scale laboratory tests. The static strength and dynamic coefficients of friction for polyester/polyester composite elements are presently studied on large-scale test equipment for determination of its bearing capacity and failure mechanisms under overload conditions. Original test samples have a diameter of 250 mm and thickness of 40 mm, corresponding to the practical implementation in the sliding surfaces of a ball-joint, and are tested at various scales for simulation of edge effects and repeatability of test results. Static tests reveal complete elastic recovery after loading to 120 MPa, plastic deformation after loading at 150 MPa and overload at 200 MPa. This makes present composite favorable for use under high loads, compared to, e.g., glass-fibre reinforced materials. Sliding tests indicate stick-slip for pure bulk composites and more stable sliding when PTFE lubricants are added. Dynamic overload occurs above 120 MPa due to an expansion of the nonconstrained top surface. A molybdenum-disulphide coating on the steel counterface is an effective lubricant for lower dynamic friction, as it favorably impregnates the composite sliding surface, while it is not effective at high loads as the coating is removed after sliding and high initial static friction is observed. Also a zinc phosphate thermoplastic coating cannot be applied to the counterface as it adheres strongly to the composite surface with consequently high initial friction and coating wear. Most stable sliding is observed against steel counterfaces, with progressive formation of a lubricating transfer film at higher loads due to exposure of PTFE lubricant. Composite wear mechanisms are mainly governed by thermal degradation of the thermosetting matrix (max. 162°C) with shear and particle detachment by the brittle nature of polyester rather than plastic deformation. The formation of a sliding film protects against fiber failure up to 150 MPa, while overload results in interlaminar shear, debonding, and ductile fiber pull-out.


1988 ◽  
Vol 110 (1) ◽  
pp. 69-72 ◽  
Author(s):  
I. L. Maksimov

The stability of sliding has been studied, taking into account frictional heating effect and friction coefficient dependence upon the interface temperature and sliding velocity. The collective—thermal and mechanical—sliding instability has been found to exist; instability emergence conditions and dynamics (both in linear and nonlinear stages) have been determined. It is shown that both the threshold and the dynamics of thermofrictional instability differ qualitatively from the analogous characteristics of “stick-slip” phenomenon. Namely, the oscillational instability behavior due to the energy exchange between thermal and mechanical modes has been found to occur under certain initial conditions; the velocities range has been determined for which collective sliding instability may occur whereas the stick-slips would be not possible. The nonlinear analysis of instability evolution has been carried out for pairs with the negative thermal-frictional sliding characteristics, the final stage of sliding dynamics has been described. It is found that stable thermofrictional oscillations can occur on the nonlinear stage of sliding instability development; the oscillations frequency and amplitude have been determined. The possibility has been discussed of the experimental observation of new dynamical sliding phenomena at low temperatures.


1988 ◽  
Vol 61 (1) ◽  
pp. 119-136 ◽  
Author(s):  
C. M. McC. Ettles ◽  
Jui Hsieh Shen

Abstract The friction of polymers and elastomers has been widely researched, both in practical applications and in fundamental experiments. Although some of the basic mechanisms of elastomer friction have been well explored, the effect of frictional heating has not received much attention. This is surprising since the low thermal conductivity of elastomers can result in quite high temperatures being generated at the interface. This paper is concerned specifically with the influence of heat generation on the level of friction at the interface. Some present theories of elastomer friction are well established. The important factors that govern friction are considered to be the strength of interface bonds and the loss tangent, tan δ, where δ is the phase lag between harmonically applied strain and the stress response. On a rough surface, friction is considered to occur from hysteretic losses. On a smooth surface, friction is considered to occur from the formation of bonds across the interface, the extension of the bonds and their eventual fracture. In several quantitative models of elastomer friction summarized by Moore and Geyer, the result for friction is directly proportional to tan δ, thus for a perfectly elastic material, the friction (according to these models) tends to approach zero. Factors affecting the interface bond strength are somewhat better understood, Schallamach proposed that the bonds were molecular. This allowed an Eyring-type rate process theory to be applied, as illustrated with great clarity by Grosch. Grosch showed that the Williams-Landel-Ferry transformation could be applied to condense the friction-speed characteristics measured at various temperatures to a single “master curve.” These experiments gave convincing evidence that rubber friction is a thermally activated, molecular kinetic, stick-slip process. Grosch's experiments were later confirmed by Ludema and Tabor.


2007 ◽  
Vol 34 (13) ◽  
pp. n/a-n/a ◽  
Author(s):  
Christophe Voisin ◽  
François Renard ◽  
Jean-Robert Grasso
Keyword(s):  

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