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reduced, flexible linear aggregates are formed. With increasing ionic strength
and decreasing charge density, the degree of branching and flexibility increases,
which enhances the local density of the aggregates. On length-scales larger than
a few tens of nanometres, the aggregates have a self-similar structure charac-
terized by a fractal dimension close to 2.
When repulsive charge interactions are important, the interpenetrating ag-
gregates and gels are highly ordered and homogeneous on length-scales larger
than a few tens of nanometres. The degree of order decreases with decreasing
electrostatic interactions, which leads to an increase of the scattered light
intensity. Beyond a certain degree of heterogeneity, the systems become turbid
to the naked eye. The increase in the heterogeneity, and therefore in the
turbidity, is strong over a narrow range of salt concentrations and pH, but
the local arrangement of the proteins varies little. A clear distinction between
the so-called fine-stranded gels and particulate gels is not justified - the
difference simply represents a gradual transition from highly ordered to very
heterogeneous gels.
Acknowledgement
Dominique Durand is thanked for fruitful discussions and a critical reading of
the manuscript.
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