Page 294 - Carbon Nanotube Fibres and Yarns
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Carbon nanotube yarn-based actuators   283


              11.5.2  Output stress (σ)
              Definition: the maximum generated force upon excitation normalized to
              the initial cross-sectional area of the actuator (engineering stress, σ E ) or the
              cross-sectional area at the excited state (true stress, σ T ).
                                               F
                                          σ =                            (11.7)
                                            E
                                               S
                                                                             2
              where F (N) is the maximum generated force upon excitation and S (m )
              is the initial cross-sectional area of the actuator. For coiled yarn actuators,
              the cross-sectional area of the coil cylinder (diameter D+2r in Fig. 11.6)
              should be used, rather than the cross-sectional area of the yarn (diameter 2r
              in Fig. 11.6).
                 For a coil actuator, if we increase the yarn strain (ε y ), for example, by hang-
              ing a heavier weight, the yarn torque Q will also increase according to Eq.
              (11.3). Consequently, the lifting force F will increase according to Eq. (11.4).
              This means that the maximum contractile stress achieved in these coils is de-
              pendent on the initial conditions, in particular the pre-strain or load applied to
              the coil at the start of the experiment. Shang et al. [55] carried out a systematic
              study on the electromechanical actuation in helical yarns stretched to a wide
              range of tensile strains. They found that the stress increased with increasing pre-
              strain up to 50%, and then decreased at larger strains (50%–130%).


              11.5.3  Energy density or work density (E)
              Definition: the output work generated by the actuator upon excitation nor-
              malized to the mass or volume of the actuator. The output work density (E)
              can be calculated using Eq. (11.8)

                             E (  J /  g) = W  or  E (  J m ) == W       (11.8)
                                                       3
                                                    /
                              m
                                                 v
                                        m
                                                             v
                                                              2
                                          2
                                         3
              where W ( J), m 2  (kg), and v 2  (m ) correspond to the output work generated
              by the actuator upon excitation, the mass of actuator, and the volume of
              actuator, respectively.
                 The easiest way to test the output work of a linear contractile actuator
              is hanging a weight and measure how high it can be lifted upon excitation.
              The contractile output work (W C ) can then be calculated using Eq. (11.9)
                                       W () =   mgh                      (11.9)
                                            J
                                                  1
                                         C
                                2
              where m 1  (kg), g (m/s ), and h (m) correspond to the mass of the object that
              is lifted by the actuator, the gravitational acceleration, and the contractive
              length of the actuator, respectively.
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