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although the fractal dimension remains at d f ¼ 2, the pre-factor a increases with
increasing ionic strength and decreasing pH. The most turbid gels that could be
studied had an average correlation length of
1 mm.
Assuming that the system can be modelled as an ensemble of close-packed
monodisperse blobs of size R a and molar mass M a , then the following equation
relates the protein concentration to R a and M a :
C E 3M a /(4N A p R a ).
B
(6)
Utilizing the relationship between M a and R a , it follows that we have R a p a 1.5
C 1 and M a p a 3 C 2 for d f ¼ 2. This result is compatible with the concen-
tration dependence of M a and R a for b-LG at 100 mM NaCl. 28 However, the
strong increase of M a at a given protein concentration with increasing ionic
strength cannot be explained by the weak increase of a. We conclude that the
gels become increasingly heterogeneous; i.e., the concentration fluctuations are
characterized by a range of correlation lengths. In terms of the blob picture, the
gels consist of an ensemble of blobs with a size distribution that increases with
decreasing electrostatic repulsion. The values of R a and M a determined by
scattering techniques represent the z-average radius and the weight-average
molar mass of the blobs, and therefore the largest blobs have a strong weight. If
the size distribution of the concentration fluctuations varies, then R a and M a
are no longer simply related to the protein concentration through the fractal
dimension. Similar observations have been made for gels formed by small clay
particles (Laponite) at different NaCl concentrations: 51 at a fixed concentra-
tion, the correlation length strongly increased with increasing ionic strength,
while the local structure remained the same.
When the length-scale of the heterogeneity approaches 1 mm, it can be
observed using CSLM, 29,43,50,52 as illustrated in Figure 12. The gels appear to
consist of aggregated micrometre-sized particles. For this reason turbid glob-
ular protein gels are often called as particle gels or particulate gels. Typically,
TEM and (particularly) SEM show a network of partly fused and roughly
spherical particles with diameters of the order of 1 mm 16,53-55
(Figure 13).
Figure 12 CSLM image of a b -LG gel formed at C ¼ 50 g L 1 ,pH ¼ 7, and 0.2 M
NaCl. 50 The total width of the image is 160 m m
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