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Charge heterogeneity induced binding and phase stability in β-lacto-globulin–gelatin B gels and coacervates at their common pI
An understanding of the interactions between gelatin B (GB) and β-lacto-globulin (β-Lg) mainly arising from surface selective patch binding occurring at their common p I (≈5.0 ± 0.5) in the absence of added salt. Heterogeneous surface charge distribution on β-Lg facilitated such interaction at diffe...
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Published in: | RSC advances 2015-01, Vol.5 (82), p.67066-67076 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | An understanding of the interactions between gelatin B (GB) and β-lacto-globulin (β-Lg) mainly arising from surface selective patch binding occurring at their common p
I
(≈5.0 ± 0.5) in the absence of added salt. Heterogeneous surface charge distribution on β-Lg facilitated such interaction at different mixing ratio ([GB]: [β-Lg] =
r
) and the GB–β-Lg complexes carried distinctive surface charge (seen through their zeta potential,
ζ
). For
r
< 1 : 1 (partial charge neutralization,
ζ
≈ 0) a turbid solution was formed which gives the indication of formation of intermolecular soluble complexes. For
r
> 1 : 1 (overcharged regime,
ζ
> 0) the dispersion remained transparent and homogeneous which gives no phase separation, but the dispersion formed a gel on waiting. The overcharged gels were homogeneous, more rigid and higher melting temperature in comparison to coacervate. In the coacervate phase, the intensity of the scattered light
I
s
, and its time-correlation function [
g
2
(
t
) − 1] did not evolve with time. In contrast, the gel phase displayed considerable change with aging time
t
w
. For gels, as
t
w
→ ∞ the system moved from an ergodic to non-ergodic state. At
t
w
= 0, the correlation function exhibited one relaxation mode due to the system residing deeply inside the ergodic phase and purely mirroring Brownian dynamics. After a characteristic waiting time,
t
w
an additional mode (slow relaxation) appeared which was attributed to inter-chain interaction induced reorganization of entanglements. This characteristic time was the time required for the system to get dynamically arrested, similar observation was made from rheology measurements too. A comprehensive phase diagram depicting the stability of the dispersion in various charged soft matter states of the complex under various temperature conditions was established. |
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ISSN: | 2046-2069 2046-2069 |
DOI: | 10.1039/C5RA07195J |