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On the structure of suspensions of charged rodlike particles

  • Application Of Colloids
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Trends in Colloid and Interface Science V

Part of the book series: Progress in Colloid & Polymer Science ((PROGCOLLOID,volume 84))

Abstract

Structural properties of colloidal suspensions of charged rodlike particles are studied by computer simulation and several perturbation theory schemes. As a model for the interaction, we consider a repulsive screened Coulomb potential between two interaction centers on each rod. — MonteCarlo simulations were performed for both the dilute (c<1/L 3) and the semidilute (c>1/L 3) regimes. Results for the pair correlation function, the static structure factor S M(k) and the angular correlation of rod axes were obtained. It turns out that the concentration dependence of the peak position of S M(k) shows a shift from a c 1/3-dependence in dilute suspensions to a c 1/2 behavior for higher concentrations as observed in light scattering experiments on suspensions of rodlike viruses. — In applying perturbation theory the full interaction potential is expanded with respect to a spherically symmetric reference potential. The latter has been determined according to several averaging schemes: mean potential, median potential, reference averaged Mayer potential (RAM) and the blip function method. A comparison of the results of these schemes with simulation data shows that perturbation theory provides a good description of the structure of this system only in the dilute regime.

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M. Corti F. Mallamace

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© 1991 Dr. Dietrich Steinkopff Verlag GmbH & Co. KG

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Weyerich, B., D’Aguanno, B., Canessa, E., Klein, R. (1991). On the structure of suspensions of charged rodlike particles. In: Corti, M., Mallamace, F. (eds) Trends in Colloid and Interface Science V. Progress in Colloid & Polymer Science, vol 84. Steinkopff, Heidelberg. https://doi.org/10.1007/BFb0116005

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  • DOI: https://doi.org/10.1007/BFb0116005

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  • Publisher Name: Steinkopff, Heidelberg

  • Print ISBN: 978-3-662-16029-9

  • Online ISBN: 978-3-7985-1685-4

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