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The interfacial interactions may be strong enough to meet this condition in special cases, such as clean metal surfaces in ultrahigh vacuum.
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Real surfaces are rarely perfect single crystals, but including disorder without third bodies does not seem to explain experimental observations. The static friction between stiff random surfaces is a finite-size effect that drops as the inverse of the contact diameter. We find that values can be appreciable on the scale of AFM tips (<40 atomic diameters), but not in micrometer-scale contacts. Elastic deformation at large scales can yield static friction, but the values are exponentially small for weak disorder (5).
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Financial support from NSF grant DMR-9634131 is gratefully acknowledged. We are also grateful to Intel for donating workstations on which these simulations were run.
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