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a) b - École Polytechnique de Montréal

a) b - École Polytechnique de Montréal

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Narkis and co-workers exten<strong>de</strong>d and <strong>de</strong>veloped previous works about melt-blending PANI and<br />

other general polymers in or<strong>de</strong>r to <strong>de</strong>crease the percolation threshold and increase mechanical<br />

properties(Haba, et al., 2000; Narkis, et al., 2000a; Segal, et al., 2001). They compared<br />

dispersion mixing (Figure 2-29a) and melt-blending process (Figure 2-29b)(Narkis, et al., 2000a)<br />

and found a percolation threshold of less than 1% for the former case and approximately 20% for<br />

latter case.<br />

a) b)<br />

Figure 2-29: Conductivity vs. concentration of PANI/polymer prepared via a) dispersion<br />

mixing, b) melt-blending(Narkis, et al., 2000a)<br />

Levon et al.(Levon, Margolina, & Patashinsky, 1993) were the first who suggested utilization of<br />

three components instead of two. They introduced the term “double percolated” in a ternary<br />

polymer blend consisting of a conductive polymer. Double percolated system was <strong>de</strong>fined as the<br />

connectivity in a hierarchical basis of a connected path within a connected path, the last of which<br />

is conducting. Narkis et al.(Narkis, et al., 2000a) reported a ternary blend comprised of<br />

(PS/DOP)/CoPA/PANI and showed that CoPA situates at the interface. They showed that PANI<br />

preferentially locates at the CoPA phase <strong>de</strong>monstrating a double percolation phenomenon in<br />

which PANI is encapsulated by CoPA. The conductivity of the blend as a function of<br />

concentration of CoPA was studied (Figure 2-30).<br />

63

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