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...
Saved in:
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.
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520 | |a 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. | ||
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500 | |a We thank O. Ben-David and J. Fineberg for numerous insightful discussions. E. B. acknowledges support of the James S. McDonnell Foundation, the Harold Perlman Family Foundation, and the Robert Rees Applied Research Fund. E. A. B. acknowledges support of the Erna and Jacob Michael visiting professorship funds at Weizmann Institute of Science. M. U. acknowledges support by the Israel Science Foundation, Grant 1109/09 and by the German-Israeli Project Cooperation Program (DIP). | ||
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