Structure/Property Relationships for Polyamide 6 / Organoclay Nanocomposites in the Melt and in the Solid State

• Published in: Macromolecular symposia. 2005-01, Vol.221 (1), p.85-94
• Main Authors: Karaman, Vitaly M., Privalko, Valery P., Privalko, Eleonora G., Lehmann, Bjorn, Friedrich, Klaus
• Format: Article
• Language: English
• Subjects: boundary interphase; clay; Clay (material); Distortion; Melts; nanocomposite; Nanocomposites; Nanoparticles; polyamide 6; Polyamide resins; Solid state; Viscosity
• ISSN: 1022-1360; 1521-3900
• DOI: 10.1002/masy.200550309

Commercial nanocomposites of polyamide 6 prepared by melt compounding with organoclays were characterized by complex viscosities and relaxation time spectra derived from storage and loss shear moduli measured in the melt state at 230°C, and by wide‐ and small‐angle X‐ray scattering, differential scanning calorimetry and stretching calorimetry in the solid state. In the melt state, the decrease of ∼ 25 % (compared to the pristine sample) in Newtonian viscosity at the lowest clay loading (2.5 %) suggested a lower equilibrium elasticity modulus of an entangled melt, as the small amounts of organoclay nanoparticles acted as specific “diluents” for the initial entanglement network. However, by increasing the clay loading this effect disappeared due to the importance of strong interactions at the nanoparticle/melt interface, leading to the formation of a fairly thick boundary interphase (BI) around the nanoparticles and ending up in the build‐up of an “infinite cluster” of clay nanoparticles coated with BI at the highest (albeit still unusually low) clay loading (7.5 %). In the solid state, organoclay nanoparticles proved to induce the crystallographic α → γ transformation of PA6 , while the matrix crystallinity in nanocomposites remained essentially unchanged. In the range of elastic (reversible) behavior below the apparent yield strains ϵ* , the highest Young's moduli E and the lowest linear thermal expansion coefficients αL were observed for dried nanocomposites, while the lowest E and the highest αL corresponded to the moisturized, pristine PA6. The endothermal process of shape distortion of the lamellar crystals was assumed to precede the onset of the exothermal process of lamellar fragmentation in the range of inelastic (irreversible) behaviour of PA6 above ϵ* . The energy balance of the inelastic behaviour of nanocomposites was dominated by the endothermal process of lamellar shape distortion.