Dynamics of Sliding Friction between Laser-Induced Periodic Surface Structures (LIPSS) on Stainless Steel and PMMA Microspheres

被引:10
作者
Cihan, Ebru [2 ,3 ]
Heier, John [1 ]
Lubig, Kevin [1 ]
Graef, Stephan [1 ]
Mueller, Frank A. [1 ]
Gnecco, Enrico [2 ,3 ,4 ]
机构
[1] Friedrich Schiller Univ Jena, Otto Schott Inst Mat Res OSIM, D-07743 Jena, Germany
[2] Tech Univ Dresden, Inst Mat Sci, D-01069 Dresden, Germany
[3] Tech Univ Dresden, Max Bergmann Ctr Biomat, D-01069 Dresden, Germany
[4] Jagiellonian Univ, Marian Smoluchowski Inst Phys, PL-30348 Krakow, Poland
关键词
AFM; stick-slip; friction; multicontact; PMMA; laser-induced periodic surface structures; stainless steel; TRIBOLOGICAL BEHAVIOR; PATTERNED SURFACES; CONTACT; RECOVERY; ENERGY;
D O I
10.1021/acsami.3c00057
中图分类号
TB3 [工程材料学];
学科分类号
0805 ; 080502 ;
摘要
In this work, we investigated the sliding friction measured between poly(methyl methacrylate) (PMMA) colloidal probes with two different diameters D (1.5 and 15 mu m) and laser induced periodic surface structures (LIPSS) on stainless steel with periodicities ? of 0.42 and 0.9 mu m, when the probes are elastically driven along two directions, perpendicular and parallel to the LIPSS. The time evolution of the friction shows the characteristic features of a reverse stick-slip mechanism recently reported on periodic gratings. The morphologies of colloidal probes and modified steel surfaces are geometrically convoluted in the atomic force microscopy (AFM) topographies simultaneously recorded with the friction measurements. The LIPSS periodicity is only revealed with smaller probes (D = 1.5 mu m) and when ? takes the largest value of 0.9 mu m. The average value of the friction force is found to be proportional to the normal load, with a coefficient of friction mu varying between 0.23 and 0.54. The values of mu are rather independent of the direction of motion, and they reach their maximum when the small probe is scanned on the LIPSS with the larger periodicity. The friction is also found to decrease with increasing velocity in all cases, which is attributed to the corresponding decrease of the viscoelastic contact time. These results can be used to model the sliding contacts formed by a set of spherical asperities of different sizes driven on a rough solid surface.
引用
收藏
页码:14970 / 14978
页数:9
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