Page 197 - Carbon Nanotube Fibres and Yarns
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Mechanics modeling of carbon nanotube yarns   187


              critical value. Such treatment led to the prediction of two strength peaks at
              α ≈ 15–20 degrees and >30 degrees, in agreement with their experimental
              results [29]. This model can be used to calculate the contribution of each
              layer of CNTs to the yarn strength. The radial pressure deep inside a CNT
              yarn is usually smaller than that near the yarn surface, in other words, the
              outer layers shield the yarn interior (“arch effect”). This was also substanti-
              ated by evidences from the yarn forming process [81].

              8.2.2  Two-scale damage mechanics model
              The above treatment is a rough model as it only extends the basic yarn ge-
              ometry to include the radial compression inside the yarn. The model cannot
              be used easily to predict the tensile behaviors of CNT yarn, such as the
              plastic deformation and failure elongation. Rong et al. [82] used a two-scale
              damage mechanics model to quantitatively investigate the effects of twisting
              on the mechanical properties of CNT yarns. They divided the component
              CNTs into two scale levels: CNT bundles that are twisted to form the yarn
              and amorphous CNT “threads” that exist in the spaces between the bundles.
              CNT threads refer to CNT groups that are much smaller than the CNT
              bundles. Upon tensioning, the CNT bundles bear most of the loads, while
              the amorphous CNT threads act as imperfect interfaces between the bundles
              for transferring shear stresses. Such treatment is reminiscent of the model
              used to describe dry-drawing of CNT sheet from a CNT forest, where the
              large-sized bundles are connected by smaller bundles or individual nano-
              tubes [83]. In the forest, the density of the small bundles plays a key role in
              determining the spinnability of a CNT forest. With increasing strain, more
              and more CNT threads are stretched and thus start to bear tensile stress. In
              the two-scale model, a CNT yarn is assumed to consist of N CNT bundles
              with a twist angle θ, in which n bundles have initiated damage. By summing
              up the contributions of these different bundles and adjusting the fractions of
              damaged bundles during tensioning, the elastic- and plastic-like behaviors of
              CNT yarns can be obtained. This treatment, although rather complicated,
              can reasonably well describe the tensioning process with the introduction of
              damage to CNT bundles.

              8.2.3  Fracture model based on intertube contacts

              The above two-scale damage mechanics model does not fully consider the
              intertube contact and shear strength, which are the most important factors
              in determining the yarn’s mechanical properties. Vilatela et al. [21] proposed
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