Department of Mechanical Engineering, Massachusetts Institute of Technology , Cambridge, Massachusetts 02139, United States.
Nano Lett. 2015 Mar 11;15(3):1503-10. doi: 10.1021/nl503641c. Epub 2015 Feb 18.
Mechanical failure of an ideal crystal is dictated either by an elastic instability or a soft-mode instability. Previous interpretations of nanoindentation experiments on suspended graphene sheets,1,2 however, indicate an anomaly: the inferred strain in the graphene sheet directly beneath the diamond indenter at the measured failure load is anomalously large compared to the fracture strains predicted by both soft-mode and acoustic analyses. Through multiscale modeling combining the results of continuum, atomistic, and quantum calculations, and analysis of experiments, we identify a strain-shielding effect initiated by mechanochemical interactions at the graphene-indenter interface as the operative mechanism responsible for this anomaly. Transmission electron micrographs and a molecular model of the diamond indenter's tip suggest that the tip surface contains facets comprising crystallographic {111} and {100} planes. Ab initio and molecular dynamics (MD) simulations confirm that a covalent bond (weld) formation between graphene and the crystallographic {111} and {100} facets on the indenter's surface can be induced by compressive contact stresses of the order achieved in nanoindentation tests. Finite element analysis (FEA) and MD simulations of nanoindentation reveal that the shear stiction provided by the induced covalent bonding restricts relative slip of the graphene sheet at its contact with the indenter, thus initiating a local strain-shielding effect. As a result, subsequent to stress-induced bonding at the graphene-indenter interface, the spatial variation of continuing incremental strain is substantially redistributed, locally shielding the region directly beneath the indenter by limiting the buildup of strain while imparting deformation to the surrounding regions. The extent of strain shielding is governed by the strength of the shear stiction, which depends upon the level of hydrogen saturation at the indenter's surface. We show that at intermediate levels of hydrogen saturation the strain-shielding effect can enable the graphene to support experimentally determined fracture loads and displacements without prematurely reaching locally limiting states of stress and deformation.
理想晶体的力学失效要么是由弹性不稳定性引起,要么是由软模不稳定性引起。然而,之前对悬浮石墨烯片的纳米压痕实验的解释表明存在异常现象:在测量的失效载荷下,直接位于金刚石压头下方的石墨烯片的推断应变异常大,与软模和声学分析预测的断裂应变相比都是如此。通过结合连续体、原子和量子计算结果的多尺度建模以及对实验的分析,我们确定了由石墨烯-压头界面的机械化学相互作用引发的应变屏蔽效应是导致这种异常现象的作用机制。透射电子显微镜和金刚石压头尖端的分子模型表明,压头表面的晶面包括{111}和{100}面。从头算和分子动力学(MD)模拟证实,在纳米压痕测试中达到的压缩接触应力下,可以在石墨烯和压头表面的晶面{111}和{100}之间形成共价键(焊接)。纳米压痕的有限元分析(FEA)和 MD 模拟表明,由诱导的共价键提供的剪切粘着限制了石墨烯片与压头接触处的相对滑动,从而引发局部应变屏蔽效应。因此,在石墨烯-压头界面上的应力诱导键合之后,连续增量应变的空间变化会得到显著重新分布,通过限制应变的积累来局部屏蔽压头正下方的区域,同时向周围区域赋予变形。应变屏蔽的程度取决于剪切粘着的强度,而剪切粘着的强度又取决于压头表面的氢饱和水平。我们表明,在中等水平的氢饱和下,应变屏蔽效应可以使石墨烯在不提前达到局部限制的应力和变形状态的情况下,支撑实验确定的断裂载荷和位移。