scholarly journals Effect of the substrate potential on the static friction force in the Frenkel-Kontorova model

2010 ◽  
Vol 59 (4) ◽  
pp. 2589
Author(s):  
Li Xiao-Li ◽  
Liu Feng ◽  
Lin Mai-Mai ◽  
Chen Jian-Min ◽  
Duan Wen-Shan
2012 ◽  
Vol 61 (13) ◽  
pp. 130501
Author(s):  
Yang Yang ◽  
Wang Cang-Long ◽  
Duan Wen-Shan ◽  
Shi Yu-Ren ◽  
Chen Jian-Min

2021 ◽  
Author(s):  
Li Yi-Wei ◽  
Xu Peng-Fei ◽  
Yang Yong-Ge

Abstract The nano-friction phenomenon in a one-dimensional Frenkel-Kontorova model under Gaussian colored noise is investigated by using the molecular dynamic simulation method. The role of colored noise is analyzed through the inclusion of a stochastic force via a Langevin molecular dynamics method. Via the stochastic Runge-Kutta algorithm, the relationship between different parameter values of the Gaussian colored noise (the noise intensity and the correlation time) and the nano-friction phenomena such as hysteresis, the maximum static friction force is separately studied here. Similar results are obtained from the two geometrically opposed ideal cases: incommensurate and commensurate interfaces. It was found that the noise strongly influences the hysteresis and maximum static friction force and with an appropriate external driving force, the introduction of noise can accelerate the motion of the system, making the atoms escape from the substrate potential well more easily. Interestingly, suitable correlation time and noise intensity give rise to super-lubricity. It is noteworthy that the difference between the two circumstances lies in the fact that the effect of the noise is much stronger on triggering the motion of the FK model for the commensurate interface than that for the Incommensurate interface.


2003 ◽  
Vol 52 (4) ◽  
pp. 879
Author(s):  
Hu Lin ◽  
Yang Ping ◽  
Xu Ting ◽  
Jiang Yang ◽  
Xu Hai-Jiang ◽  
...  

2002 ◽  
Vol 12 (9) ◽  
pp. 319-320
Author(s):  
T. Nitta ◽  
H. Haga ◽  
K. Kawabata

We measured the static friction force of agar gel-on-glass plate in water. The static friction force is independent of the apparent contact area between the agar gel and the glass plate. It increases with waiting time, that is, contact duration prior to motion. The static friction force is represented well by a power law of waiting time. The waiting time dependence is different from those of solid-on-solid systems. These results are discussed, based on asperity contact model.


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