Li Suzhi, Li Qunyang, Carpick Robert W, Gumbsch Peter, Liu Xin Z, Ding Xiangdong, Sun Jun, Li Ju
State Key Laboratory for Mechanical Behavior of Materials and Frontier Institute of Science and Technology, Xi'an Jiaotong University, Xi'an 710049, China.
Department of Nuclear Science and Engineering and Department of Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.
Nature. 2016 Nov 24;539(7630):541-545. doi: 10.1038/nature20135.
Graphite and other lamellar materials are used as dry lubricants for macroscale metallic sliding components and high-pressure contacts. It has been shown experimentally that monolayer graphene exhibits higher friction than multilayer graphene and graphite, and that this friction increases with continued sliding, but the mechanism behind this remains subject to debate. It has long been conjectured that the true contact area between two rough bodies controls interfacial friction. The true contact area, defined for example by the number of atoms within the range of interatomic forces, is difficult to visualize directly but characterizes the quantity of contact. However, there is emerging evidence that, for a given pair of materials, the quality of the contact can change, and that this can also strongly affect interfacial friction. Recently, it has been found that the frictional behaviour of two-dimensional materials exhibits traits unlike those of conventional bulk materials. This includes the abovementioned finding that for few-layer two-dimensional materials the static friction force gradually strengthens for a few initial atomic periods before reaching a constant value. Such transient behaviour, and the associated enhancement of steady-state friction, diminishes as the number of two-dimensional layers increases, and was observed only when the two-dimensional material was loosely adhering to a substrate. This layer-dependent transient phenomenon has not been captured by any simulations. Here, using atomistic simulations, we reproduce the experimental observations of layer-dependent friction and transient frictional strengthening on graphene. Atomic force analysis reveals that the evolution of static friction is a manifestation of the natural tendency for thinner and less-constrained graphene to re-adjust its configuration as a direct consequence of its greater flexibility. That is, the tip atoms become more strongly pinned, and show greater synchrony in their stick-slip behaviour. While the quantity of atomic-scale contacts (true contact area) evolves, the quality (in this case, the local pinning state of individual atoms and the overall commensurability) also evolves in frictional sliding on graphene. Moreover, the effects can be tuned by pre-wrinkling. The evolving contact quality is critical for explaining the time-dependent friction of configurationally flexible interfaces.
石墨和其他层状材料被用作宏观金属滑动部件和高压触点的干润滑剂。实验表明,单层石墨烯比多层石墨烯和石墨表现出更高的摩擦力,并且这种摩擦力会随着持续滑动而增加,但其背后的机制仍存在争议。长期以来,人们一直推测两个粗糙物体之间的真实接触面积控制着界面摩擦。真实接触面积,例如由原子间力范围内的原子数量定义,很难直接可视化,但它表征了接触的数量。然而,越来越多的证据表明,对于给定的一对材料,接触质量会发生变化,并且这也会强烈影响界面摩擦。最近,人们发现二维材料的摩擦行为表现出与传统块状材料不同的特征。这包括上述发现,即对于少层二维材料,静摩擦力在达到恒定值之前的最初几个原子周期内会逐渐增强。这种瞬态行为以及稳态摩擦力的相关增强随着二维层数的增加而减弱,并且仅在二维材料松散地附着在基板上时才会观察到。这种与层数相关的瞬态现象尚未被任何模拟所捕捉。在这里,我们使用原子模拟再现了石墨烯上与层数相关的摩擦和瞬态摩擦增强的实验观察结果。原子力分析表明,静摩擦力的演变是较薄且约束较少的石墨烯由于其更大的柔韧性而重新调整其构型的自然趋势的体现。也就是说,尖端原子被更强烈地固定,并且在其粘滑行为中表现出更大的同步性。虽然原子尺度接触的数量(真实接触面积)在演变,但质量(在这种情况下,单个原子的局部固定状态和整体适配性)在石墨烯上的摩擦滑动中也在演变。此外,这些效应可以通过预褶皱来调节。不断演变的接触质量对于解释构型灵活界面的时间依赖性摩擦至关重要。