CRACK Agilent ADS 2009 Update 1 |TOP| ➝
November 29, 2022
CRACK Agilent ADS 2009 Update 1
a wearable strain gauge was attached to the graphene to measure the strain distribution on the graphene at the crack tip. under a tensile load, the graphene was stretched and yielded at the crack tip, resulting in the distortion of the strain gauge (fig. 3g ). it is found that the maximum strain of the graphene is less than 0.1%, which is lower than that of the pdms (~10%). this is expected, because the graphene is much stiffer than pdms. the strain gauge response is shown in fig. 3h.
the crack tip instability can be studied by 3d atomic force microscopy (afm) imaging. a typical afm image of a crack tip is shown in fig. 4a. the crack tip is about a few micrometers long and its edges are atomically sharp. figure 4b shows the crack tip profile from the image along the dashed line in fig. from the profile, the crack tip velocity can be obtained, which is about 10-6m/s. based on the crack tip velocity, the time required to reach the critical crack length is about 10ms. compared to the case of graphene on pdms, a higher crack tip velocity is observed. although the crack tip is more stable in graphene/pdms, it is much more difficult to capture the crack tip using afm. this could be due to the fact that the pdms is viscous and no viscoelastic material is used in the crack tip profile experiment. the crack tip is thus able to move away from the afm tip if the pdms is not viscous enough. this is also demonstrated by the large deformation of the graphene when pdms is peeled off (see fig. 4c ), which indicates that graphene is quite sensitive to the surrounding environment and is not robust enough for more complicated crack tip profiles.
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