Numéro |
J. Phys. II France
Volume 5, Numéro 5, May 1995
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Page(s) | 677 - 695 | |
DOI | https://doi.org/10.1051/jp2:1995157 |
J. Phys. II France 5 (1995) 677-695
Flory Theory of a Polyampholyte Chain
Andrey V. Dobrynin1 and Michael Rubinstein21 Department of Physics and Astronomy, Unversity of Rochester, Rochester, New York 14627-0011, USA
2 Imaging Research and Advanced Development, Eastman Kodak Company, Rochester, New York 14650-02116, USA
(Received 8 August 1995, revised 12 January 1995, accepted 8 February 1995)
Abstract
The behavior of a polyampholyte chain is analyzed in the framework of the two-parameter Flory theory. We consider a
N-mer containing
N+ positively charged monomers and
N- negatively charged ones. There are three different regimes for polyampholytes with charge asymmetry
|N+ -N-|>(N+ +N-)1/2 depending on the effective temperature
, where
u is the ratio of the Bjerrum length
to the bond size
b: (i) Unperturbed regime: at high effective temperatures
t>t1 the electrostatic interactions are unimportant and polyampholyte configuration is controlled by the solvent quality for the
uncharged backbone, (ii) Polyelectrolyte regime: at intermediate effective temperatures
t2<t<t1 the repulsion between uncompensated charges
e(N+-N-) dominates over the charge-fluctuation-induced attraction. The chain is stretched into an array of electrostatic blobs, (iii)
Polyampholyte regime
(t<t2): when the Debye screening length due to the charges on the chain becomes smaller than the electrostatic blob size, the charge-fluctuation-induced
attraction collapses the polyampholyte into an elongated globule with aspect ratio
independent of the temperature. The nearly symmetric chains with
directly cross over from regime (i) to regime (iii), but stay nearly spherical.
© Les Editions de Physique 1995