This title appears in the Scientific Report :
2008
Please use the identifier:
http://dx.doi.org/10.1088/09538984/20/39/395006 in citations.
On the origin of Amonton's friction law
On the origin of Amonton's friction law
Amonton's law states that the sliding friction force increases linearly with the load. We show that this result is expected for stiff enough solids, even when the adhesional interaction between the solids is included in the analysis. As a function of the magnitude of the elastic modulus E, one...
Personal Name(s):  Persson, B. N. J. 

Sivebaek, I. M. / Samoilov, V. N. / Zhao, K. / Volokitin, A. I. / Zhang, Z.  
Contributing Institute: 
QuantenTheorie der Materialien; IFF1 
Published in:  Journal of physics / Condensed matter, 20 (2008) S. 395006 
Imprint: 
Bristol
IOP Publ.
2008

Physical Description: 
395006 
DOI: 
10.1088/09538984/20/39/395006 
Document Type: 
Journal Article 
Research Program: 
Kondensierte Materie 
Series Title: 
Journal of Physics: Condensed Matter
20 
Subject (ZB):  
Publikationsportal JuSER 
Amonton's law states that the sliding friction force increases linearly with the load. We show that this result is expected for stiff enough solids, even when the adhesional interaction between the solids is included in the analysis. As a function of the magnitude of the elastic modulus E, one can distinguish between three regions: (a) for E > E2, the area of real contact (and the friction force) depends linearly on the load, (b) for E1 < E < E2, the area of real contact depends nonlinearly on the load but vanishes for zero load, and (c) for E < E1 the area of real contact depends nonlinearly on the load and is nonvanishing at zero load. In this last case a finite pulloff force is necessary in order to separate the solids. Based on molecular dynamics calculations, we also discuss the pressure dependence of the frictional shear stress for polymers. We show that the frictional shear stress is independent of the normal pressure p(0) as long as p(0) is much smaller than the adhesional pressure p(ad), which depends on the atomic corrugation of the solid surfaces in the sliding interface. Finally, we discuss the origin of why the contact area between a soft elastic solid (e. g. rubber) and a flat substrate decreases from the JKR (adhesive contact) limit at zero or small sliding velocities, to the Hertz (nonadhesive) limit at high sliding velocities. 