This title appears in the Scientific Report :
2011
Please use the identifier:
http://hdl.handle.net/2128/7390 in citations.
Please use the identifier: http://dx.doi.org/10.1103/PhysRevLett.107.235501 in citations.
Slow cracklike dynamics at the onset of frictional sliding
Slow cracklike dynamics at the onset of frictional sliding
We propose a friction model which incorporates interfacial elasticity and whose steady state sliding relation is characterized by a generic nonmonotonic behavior, including both velocity weakening and strengthening branches. In 1D and upon the application of sideway loading, we demonstrate the exist...
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Personal Name(s): | Bouchbinder, E. |
---|---|
Barel, I. / Brener, E.A. / Urbakh, M. | |
Contributing Institute: |
Theoretische Nanoelektronik; PGI-2 |
Published in: | Physical review letters, 107 (2011) S. 235501 |
Imprint: |
College Park, Md.
APS
2011
|
Physical Description: |
235501 |
DOI: |
10.1103/PhysRevLett.107.235501 |
Document Type: |
Journal Article |
Research Program: |
Grundlagen für zukünftige Informationstechnologien |
Series Title: |
Physical Review Letters
107 |
Subject (ZB): | |
Link: |
Get full text OpenAccess |
Publikationsportal JuSER |
Please use the identifier: http://dx.doi.org/10.1103/PhysRevLett.107.235501 in citations.
We propose a friction model which incorporates interfacial elasticity and whose steady state sliding relation is characterized by a generic nonmonotonic behavior, including both velocity weakening and strengthening branches. In 1D and upon the application of sideway loading, we demonstrate the existence of transient cracklike fronts whose velocity is independent of sound speed, which we propose to be analogous to the recently discovered slow interfacial rupture fronts. Most importantly, the properties of these transient inhomogeneously loaded fronts are determined by steady state front solutions at the minimum of the sliding friction law, implying the existence of a new velocity scale and a "forbidden gap" of rupture velocities. We highlight the role played by interfacial elasticity and supplement our analysis with 2D scaling arguments. |