1994
DOI: 10.1103/physreve.49.4973
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Creep, stick-slip, and dry-friction dynamics: Experiments and a heuristic model

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Cited by 539 publications
(587 citation statements)
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“…9F=9 ¿ 0 is agreeable enough, and 9F=9V ¿ 0 is a ÿrmly established experimental result (Dieterich, 1979;Tullis and Weeks, 1986;Heslot et al, 1994;Marone, 1998), re ecting the positive instantaneous velocity dependence of processes at asperity contacts. 9F=9 ¿ 0 merely sets a convention for the state variable; larger values mean greater strength, which is consistent with the usual interpretation of as a measure of the average maturity of the asperity contact population (more mature contacts are stronger).…”
Section: General Rate and State Framework Including Variable Normal supporting
confidence: 54%
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“…9F=9 ¿ 0 is agreeable enough, and 9F=9V ¿ 0 is a ÿrmly established experimental result (Dieterich, 1979;Tullis and Weeks, 1986;Heslot et al, 1994;Marone, 1998), re ecting the positive instantaneous velocity dependence of processes at asperity contacts. 9F=9 ¿ 0 merely sets a convention for the state variable; larger values mean greater strength, which is consistent with the usual interpretation of as a measure of the average maturity of the asperity contact population (more mature contacts are stronger).…”
Section: General Rate and State Framework Including Variable Normal supporting
confidence: 54%
“…It is now generally assumed to be descended from an Arrhenius activated rate process describing creep at asperity contacts. That interpretation had been mentioned earlier by Stesky (1977), was implicit in Chester (1994), and was suggested explicitly, in the rate and state framework, by Heslot et al (1994), Brà echet and Estrin (1994), Baumberger (1997), Sleep (1997), Persson (1998), Baumberger et al (1999), Lapusta et al (2000), and Nakatani (2001). In such an interpretation, for the simple case of a single activated process, we write the slip rate as…”
Section: Physical and Empirical Basis For Standard Rate And State Lawsmentioning
confidence: 78%
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“…Several dynamic processes of physical [1], geologic [2], and technological [3] interest involve superposed interacting rough surfaces able to display stick-slip motion [4]. It has been discovered in the last few years that the intermittent sliding or stick-slip dynamics of a rough solid cylinder on a rough inclined surface submitted to small controlled perturbations is a fluctuation phenomenon characterized by non-trivial spatiotemporal scaling laws [5,6], and complex critical exponents [7] if the inclination is below the angle of repose.…”
Section: Introductionmentioning
confidence: 99%