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Charge heterogeneity induced binding and phase stability in β-lacto-globulin-gelatin B gels and coacervates at their common pIElectronic supplementary information (ESI) available: UV-Vis absorbance spectra and Cole-Cole plot for different mixing ratios of β-Lg and gelatin B undertaken in this study are included in the Supplementary information. See DOI: 10.1039/c5ra07195j

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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Main Authors: Pathak, Jyotsana, Rawat, Kamla, Bohidar, H. B
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description 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. 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.
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For r &gt; 1 : 1 (overcharged regime, ζ &gt; 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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For r &lt; 1 : 1 (partial charge neutralization, ζ 0) a turbid solution was formed which gives the indication of formation of intermolecular soluble complexes. For r &gt; 1 : 1 (overcharged regime, ζ &gt; 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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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. 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.</abstract><doi>10.1039/c5ra07195j</doi><tpages>11</tpages></addata></record>
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title Charge heterogeneity induced binding and phase stability in β-lacto-globulin-gelatin B gels and coacervates at their common pIElectronic supplementary information (ESI) available: UV-Vis absorbance spectra and Cole-Cole plot for different mixing ratios of β-Lg and gelatin B undertaken in this study are included in the Supplementary information. See DOI: 10.1039/c5ra07195j
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