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Electromechanical characterization of magnetic responsive and conductive  355



                                    3000

                                    2500
                                  Conductivity (S/cm)  1500
                                    2000




                                    1000

                                     500

                                       0
                                            0      1     2      3     4      5
                                                Ratio of PEDOT:PSS to Fe 3 O 4  (1:x)

                                                    Figure 15.4
                                        Conductivity versus ratio of Fe 3 O 4 NPs.




                         Table 15.2: Fracture strength and elongation at break of composite films.
                       Sample                   Fracture strength (MPa)  Elongation at break (%)
                       1:1 without DMSO and xyl  49.0                  11.2
                       1:1 with DMSO and xyl    39.3                   39.2
                       1:5 with DMSO and xyl    42.0                   20.7



               allowing for various possible applications. It is observed that 1:5 samples have a lower
               value of elongation at break than 1:1. As a higher amount of stable Fe 3 O 4 NPs is dispersed
               within the polymer matrix, the films become increasingly brittle. Hence, the fracture
               strength is lower than that of the 1:1 sample (Figs. 15.5 and 15.6).

               15.3.3 Magnetic properties of PEDOT:PSS/xylitol/Fe 3 O 4 films

               The magnetic properties of the PEDOT:PSS/xylitol/Fe 3 O 4 films with various weight ratios
               of Fe 3 O 4 NPs have been examined by studying the M-H curve, where the magnetization is
               represented by M, and the magnetic field is represented by H (Figs. 15.7 and 15.8). All
               experiments were conducted at room temperatures. Minimum hysteresis is observed for the
               1:5 samples, which are well fitted to the theoretical model indicating its superparamagnetic
               ability. The hysteresis loops for the composite films have been measured using a VSM at
               room temperature. As can be seen from Table 15.3, the coercivity of the samples remains
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