Static and Kinetic Friction in Frenkel-Kontorova-like Models. Franz-Josef Elmer University of Basel Switzerland
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1 Static and Kinetic Friction in Frenkel-Kontorova-like Models Franz-Josef Elmer University of Basel Switzerland
2 Friction in Frenkel-Kontorova-like Models 1 Overview 1. The Frenkel-Kontorova (FK) Model 2. The Frenkel-Kontorova-Tomlinson (FKT) Model 3. Static friction 4. Kinetic friction 5. Pinning Sliding 6. Why studying toy models?
3 Friction in Frenkel-Kontorova-like Models 2 1. The Frenkel-Kontorova (FK) Model Equation of motion: ẍ j +γẋ j = x j 1 + x j+1 2x j b sin x j +F, j = 1,..., N Boundary conditions: x j+n = x j + 2πM, averaged distance: a = 2π M N
4 Friction in Frenkel-Kontorova-like Models 3 2. The Frenkel-Kontorova-Tomlinson (FKT) Model Equation of motion: ξ j + (γ L + γ U ) }{{} γ Boundary conditions: ξ j = ξ j 1 +ξ j+1 (2+κ)ξ j +b sin 2π ( x B {}}{ vt +cj + ξ j ), j = 1,..., N x j }{{} ξ j+n = ξ j, c = M N
5 Friction in Frenkel-Kontorova-like Models 4 Co-workers: Torsten Strunz, Michael Weiss Publications FK model: 1. T. Strunz and F.J. Elmer, Phys. Rev. E 58, 1601 (1998). 2. T. Strunz and F.J. Elmer, Phys. Rev. E 58, 1612 (1998). Publications FKT model: 1. M. Weiss and F.J. Elmer, Phys. Rev. B. 53, 7539 (1996). 2. M. Weiss and F.J. Elmer, Z. Phys. B. 104, 55 (1997). 3. F.J. Elmer, in Workshop on Friction, Arching, Contact Dynamics edited by D. E. Wolf and P. Grassberger (World Scientific, Singapore, 1997).
6 Friction in Frenkel-Kontorova-like Models 5 3. Static friction Phenomenological definition:the force necessary to start sliding. Static friction depends on history, inertia, and temperature. Unique definition: Static friction F S is the force where the last (meta)stable state disappears.
7 Friction in Frenkel-Kontorova-like Models 6 Properties of the static friction in FK and FKT model 1. Ground state at F = 0 last state at F = F S 2. Commensurate lattic constants: FKT model, κ = 1 F S b Q c golden mean where Q = N/gcd(M, N). 3. Incommensurate lattic constants: { 0 : b < b F S = S c const (b b S c ) α : b > b S c with α = 3 for FK and α = 2 for FKT.
8 Friction in Frenkel-Kontorova-like Models 7 4. Kinetic friction Definition: The averaged force F K necessary to slide with an on average constant velocity v. Dissipated energy per time unit: F K v Averaged kinetic friction: F = F K N = γ L + γ (ẋj v 1 with the averaged velocity v = ẋj j t ) 2 j t v Dissipation channels:
9 Friction in Frenkel-Kontorova-like Models 8 Kinetic friction versus velocity:
10 Friction in Frenkel-Kontorova-like Models 9 How uniform motion excites phonons? The periodic substrate acts like a wave: washboard wave: phonon: wavenumber K, frequency Ω v wavenumber k, frequency ω(k) Dispersion relation: FK model: ω(k) = 2 sin(k/2) FKT model: ω(k) = κ + 4 sin 2 (k/2) Resonances: Main resonance: Superharmonic resonance of 2. order: Parametric resonance of 1. order: k 1, ω 1 k 2, ω 2
11 Friction in Frenkel-Kontorova-like Models 10 Resonances in the kinetic friction F K : FK model FKT model
12 Friction in Frenkel-Kontorova-like Models 11 Kinetic friction in the FKT model in the small velocity limit commensurate case: b < b K c b > b K c incommensurate case: b < b S c b > b S c
13 Friction in Frenkel-Kontorova-like Models Pinning Sliding Pinning sliding transition: Happens at a saddle-node bifurcation Usually starts at a certain particle Leads to an avalanche involving neighbouring particles Microslip: Avalanche stops before sweeping over all particles Pinning sliding transition: A system-spanning avalanche
14 Friction in Frenkel-Kontorova-like Models 13 Microslip in the FK model
15 Friction in Frenkel-Kontorova-like Models 14 Sliding pinning transition in the FK model Similar to an ordinary first order phase transition: 1. creation of a critical nucleus: nucleation time t N is Poisson-distributed t N = t N 1/N 2. growth of the nucleus: growth time t G t G N
16 Friction in Frenkel-Kontorova-like Models Why studying toy models? Or in terms of todays question in the Round Table Discussion: Are abstract models useful for anything? Yes, because toy models are conceptual simple laboratories for basic concepts analytical treatable, at least sometimes ;-) less expensive for simulation (a PC instead of a super computer is enough)
17 Friction in Frenkel-Kontorova-like Models 16 The Friction Lab The FK model as a Java Applet. Other models in the future.
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