Polyelectrolyte theory. I. Counterion accumulation, site‐binding, and their insensitivity to polyelectrolyte shape in solutions containing finite salt concentrations

We have computed the Poisson‐Boltzmann distribution of counterions around polyelectrolytes in solutions containing finite salt concentrations. The polyelectrolytes considered here are highly charged in the sense that ξ > 1, ξ being the linear charge density parameter for cylinders, which is generalized by us to other shapes.

[1]  G. Weisbuch,et al.  Polyelectrolyte theory. 2. Activity coefficients in Poisson-Boltzmann and in condensation theory. The polarizability of the counterion sheath , 1979 .

[2]  H. Wennerström,et al.  Ion condensation on planar surfaces. A solution of the Poisson-Boltzmann equation for two parallel charged plates , 1978 .

[3]  D. Stigter A comparison of Manning's polyelectrolyte theory with the cylindrical Gouy model , 1978 .

[4]  T. Lohman,et al.  Thermodynamic analysis of ion effects on the binding and conformational equilibria of proteins and nucleic acids: the roles of ion association or release, screening, and ion effects on water activity , 1978, Quarterly Reviews of Biophysics.

[5]  G. S. Manning The molecular theory of polyelectrolyte solutions with applications to the electrostatic properties of polynucleotides , 1978, Quarterly Reviews of Biophysics.

[6]  D. Stigter On the invariance of the charge of electrical double layers under dilution of the equilibrium electrolyte solution , 1978 .

[7]  Charles Anderson,et al.  Sodium-23 NMR studies of cation-DNA interactions. , 1978, Biophysical chemistry.

[8]  M. Guéron,et al.  Electrostatic effects in divalent ion binding to tRNA , 1977, Biopolymers.

[9]  G. S. Manning Limiting laws and counterion condensation in polyelectrolyte solutions. IV. The approach to the limit and the extraordinary stability of the charge fraction. , 1977, Biophysical chemistry.

[10]  J. Schellman,et al.  Electrical double layer, zeta potential, and electrophoretic charge of double‐stranded DNA , 1977, Biopolymers.

[11]  K. Iwasa,et al.  The contribution of higher order cluster terms to the activity coefficients of the small ions in polyelectrolyte solutions , 1977 .

[12]  H. Gregor,et al.  Coulombic reactions of polyelectrolytes with counterions of different sizes , 1977 .

[13]  R. Koren,et al.  Magnetic resonance and kinetic studies of the role of the divalent cation activator of RNA polymerase from Escherichia coli. , 1977, Biochemistry.

[14]  D. Stigter The charged colloidal cylinder with a gouy double layer , 1975 .

[15]  J. Leyte,et al.  Reply: ’’Nuclear magnetic relaxation of 23Na in polyelectrolyte solutions’’ , 1974 .

[16]  A. Macgillivray Lower Bounds on Solutions of the Poisson‐Boltzmann Equation near the Limit of Infinite Dilution , 1972 .

[17]  Gerald S. Manning,et al.  Limiting Laws and Counterion Condensation in Polyelectrolyte Solutions I. Colligative Properties , 1969 .

[18]  P. Ross,et al.  Electrophoresis of DNA. II. Specific interactions of univalent and divalent cations with DNA , 1964 .

[19]  M. Nagasawa,et al.  Chain Model for Polyelectrolytes. VII. Potentiometric Titration and Ion Binding in Solutions of Linear Polyelectrolytes , 1962 .

[20]  P. Ander,et al.  A Simple Interpretation of Donnan Equilibria Obtained with Long Chain Polyphosphates1 , 1958 .

[21]  G. Scatchard,et al.  Physical Chemistry of Protein Solutions. V. The Combination of Human Serum Albumin with Thiocyanate Ion1a , 1950 .