Results and discussion Determination

of CCI-779 mouse minimum wear depth In the friction process, there are three force components acting on the probe, as scratching force along X direction, penetration force along Y direction, and lateral force along Z direction, respectively. In the penetration stage, both scratching force and lateral force mainly fluctuate around constant value of 0 because the probe only applies uniaxial localized stress along Y direction. Figure 2 plots the penetration force-penetration depth curve during the penetration stage with a probe radius of 8 nm, indicating that the deformation behavior of the substrate is divided into two regimes. In the regime I, the substrate undergoes elastic deformation, accompanied with rapid increase of the penetration force. After the penetration depth reaches a critical value of 0.72 nm, the penetration force drops precipitously, indicating the occurrence of elastic deformation-plastic LY2606368 solubility dmso deformation transition. The observed phenomenon of force drop, which corresponds to the pop-in event widely observed in the load-controlled nanoindentation experiments, is caused by dislocation www.selleckchem.com/products/erastin.html avalanche beneath the penetrated surface [5, 7, 24]. We note that the tribochemistry, e.g., the presence of cupric oxide, may significantly

alter the deformation behavior of the topmost surface. In the regime II, the substrate undergoes plastic deformation dominated by dislocation activities. The action of penetration stops at a penetration depth D2 of 0.82 nm. Another penetration depth D1 of 0.65 nm in the elastic deformation regime, at which the penetration force is equal to that at D2, is also marked in Figure 2. The two insets in Figure 2 present instantaneous defect structures obtained at the two penetration depths D1 and D2, respectively. While the substrate is purely elastically deformed at D1, there is a considerable amount of defects formed beneath the penetrated surface at D2. Figure 2 Penetration force-penetration depth curve during the penetration

with a probe radius of 8 nm. The two penetration depths D1 of 0.65 nm and D2 of 0.82 nm have the same penetration force. The two insets show instantaneous defect structures at D1 and D2, in which atoms are colored according to their BAD values and FCC atoms are not shown. While Figure 2 shows that the defect structures at the two penetration depths are significantly Interleukin-3 receptor different, two scratching simulations under the two scratching depths D1 and D2 are conducted with the same probe radius of 8 nm. Under the scratching depth D1, both the penetration force and scratching force remain constant values throughout the scratching stage. However, the scratching force is far smaller than the penetration force because of the absence of permanent deformation in the vicinity of the probe. We also note that the non-adhesion between the substrate and the probe in the current simulated system also contributes to the ultra-small scratching force.