Conducting Polyaniline Nanoparticle Blends with Extremely Low

Apr 15, 1995 - extremly low percolation threshold cf,) in every case. The volume fraction of PANI-HC1 at the percolation threshold for the above menti...
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Macromolecules 1995,28, 3940-3943

Conducting Polyaniline Nanoparticle Blends with Extremely Low Percolation Thresholds Pallab Banerjee and Broja M. Mandal* Polymer Science Unit, Indian Association for the Cultivation of Science, Jadavpur, Calcutta 700 032, India Received December 13, 1994; Revised Manuscript Received March 3, 1995@

ABSTRACT: Blends of HC1-doped polyaniline (PANI-HC1)nanoparticles with the following conventional polymers, poly(viny1chloride), polystyrene, poly(methy1methacrylate), poly(viny1acetate), and poly(viny1 alcohol) (PVA), were prepared by suspending preformed submicronic PANI-HC1particles in the solutions of the matrix polymers and sonicating the suspension for 1.5 h. The submicronic PANI-HC1 particles were prepared by oxidative dispersion polymerization using poly(viny1 methyl ether) (PVME) stabilizer. The particles contained 4.4 w t % PVME and had a conductivity of 4.96 Slcm. They had a n oblong shape (250 nm x 190 nm). Sonication breaks the particles t o sizes less than 20 nm. The blend films exhibit an extremly low percolation threshold cf,) in every case. The volume fraction of PANI-HC1at the percolation threshold for the above mentioned matrices lies in the range 2.5 x to 4 x Transmission electron microscoopy of PANI-HC1-PVA blend films directly cast on carbon-coated TEM grids reveals connectivity at compositions close to f,. Self-assembly of the nanoparticles is evident from the TEM pictures.

Introduction There has been considerable interest in recent years on conducting polymer blends with low percolation thresholds.1-8 These materials, besides being conductive, processable, technologically attractive by virtue of being transparent, cost effective, and mechanically as strong as the matrix polymer, have been subjects of scientific curiosity with regard to their morphology and electron transport properties. The classical percolation theory predicts the percolation threshold at a volume fraction f , = 0.16 for conducting particles dispersed in an insulating matrix in three dimension^.^ This prediction is found to be true with some conducting polymer blends.1°-12 However, of late, some success in making conducting polymer blends with f p