Page 286 - Carbon Nanotube Fibres and Yarns
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Carbon nanotube yarn-based actuators   275



























              Fig. 11.3  SEM images of (A) single-ply twisted yarn, (B) two-ply twisted yarn, (C) single
              coiled yarn, (D) two-ply coiled yarn [41], and (E) five-ply coiled left-handed yarn [42].
              (Source of (A–D): J.A. Lee, Y.T. Kim, G.M. Spinks, D. Suh, X. Lepró, M.D. Lima, R.H. Baughman,
              S.J. Kim, All-solid-state carbon nanotube torsional and tensile artificial muscles, Nano Lett.
              14 (5) (2014) 2664–2669. Source of (E): P. Chen, S. He, Y. Xu, X. Sun, H. Peng, Electromechanical
              actuator ribbons driven by electrically conducting spring-like fibers, Adv. Mater. 27 (34)
              (2015) 4982–4988.)
                 Obviously, several single yarns can be combined to form a torque-free
              multiply yarn. Coiled yarns (cylindrical snarls) can also be reverse-twisted
              into a torque-free multiply yarn. Fig. 11.3 shows these different structures
              formed from CNT single yarns and coils.


              11.3  Actuator architectures
              11.3.1  Tensile actuators—Twist spun yarns

              Electrodes made from sheets of single-walled carbon nanotubes (SWCNT)
              [3] and multiwalled CNTs [14] filled with electrolytes was used to generate
              contraction, as illustrated in Fig. 11.4. Changing the applied voltage injects
              electronic charge into the CNT electrode, which is compensated at the
              nanotube-electrolyte interface by electrolyte ions (forming the so-called
              double layer). The charge injection originated from quantum chemical and
              double-layer electrostatic effects cause changes of the CC bond length.
              The strain generated on CNT sheets is quite small, in the order of 0.2%.
                 When the CNT sheets are replaced by twisted CNT yarns, strains of up
              to 0.5% can be obtained in response to an applied potentials of 2.5 V [43]. As
              shown by Eqs. (11.1) and (11.2), if we tether the two ends of a twist-spun
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