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                    270                                     Biomimetics: Biologically Inspired Technologies

                    requirement for drive voltages as low as 1 to 2 V. However, it is necessary to maintain wetness, and
                    except for conductive polymers and carbon nanotubes it is difficult to sustain DC-induced dis-
                    placements. The induced displacement of both the electronic and ionic EAP can be geometrically
                    designed to bend, stretch, or contract. Any of the existing EAP materials can be made to bend with a
                    significant curving response, offering actuators with an easy to see reaction and an appealing
                    response. However, bending actuators have relatively limited applications due to the low force or
                    torque that can be induced.



                                     10.3  TYPES OF ELECTROACTIVE POLYMERS

                    The types of EAP in each of the two material groups are given below:

                    10.3.1 Electronic EAP

                    The electronic types of EAP consist of materials that are squeezed by the attraction force between
                    the charged electrodes. Some materials in this group are internally affected to augment the
                    squeezing effect. The dielectric elastomer sustains a deformation under the stress induced by the
                    electric field driven by Maxwell Forces (Zhang et al., 2004). The other type of electronic EAP
                    materials is internally active and sustains realignment of the molecular structure (e.g., pendant
                    group on a backbone chain) or shift of atoms in the crystallographic structure in response to the
                    field. The electronic type of EAP materials include:

                    10.3.1.1 Dielectric Elastomer EAP

                    Polymers with low elastic stiffness and high dielectric breakdown strength can be used to produce a
                    large actuation strain by subjecting them to an electrostatic field. Such EAP materials also known as
                    dielectric elastomer EAP can be represented by a parallel plate capacitor as shown in Figure 10.1
                    (Pelrine et al., 1998; Kornbluh et al., 2004). The electrodes are highly compliant so as not to impede
                    the deformation of the film. The strain that results from applying an electric field is proportional to
                    the square of the electric field square, multiplied by the dielectric constant, and it is inversely
                    proportional to the elastic modulus. To reach the required electric field levels, one needs to use high
                    voltage or employ thin films or both. Under an electric field, the film is squeezed in the thickness
                    direction, causing expansion in the transverse planar direction.
                       The above characteristic allows for the production of linear actuators using dielectric elastomer
                    films that appear to act similar to biological muscles. For this purpose, SRI International scientists
                    constructed actuators using two elastomer layers with carbon electrodes on both sides of one of the
                    layers, where the layers were rolled to form a cylindrical actuator. The rolled actuator expands
                    longitudinally as a result of the Poisson effect of transverse expansion of the film that is caused by
                    its being squeezed by Maxwell Forces. Thereby, the lateral expansion leads to a lateral stretch of the



                                  + Electrode







                                 − Electrode
                    Figure 10.1  Under electric field a dielectric elastomer with electrodes on both surfaces expands laterally.
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