Colloidal gels formed by colloid–polymer mixtures with an intermediate volume fraction (fc E 0.4) are investigated by confocal microscopy. In addition, we have performed Monte Carlo simulations based on a simple effective pair potential that includes a short-range attractive contribution representing depletion interactions, and a longer-range repulsive contribution describing the electrostatic interactions due to the presence of residual charges. Despite neglecting non-equilibrium effects, experiments and simula- tions yield similar gel structures, characterised by, e.g., the pair, angular and bond distribution functions. We find that the structure hardly depends on the strength of the attraction if the electrostatic contribu- tion is fixed, but changes significantly if the electrostatic screening is changed. This delicate balance between attractions and repulsions, which we quantify by the second virial coefficient, also determines the location of the gelation boundary.

Structure of colloidal gels at intermediate concentrations: the role of competing interactions / Capellmann R.F.; Valadez-Perez N.E.; Simon B.; Egelhaaf S.U.; Laurati M.; Castaneda-Priego R.. - In: SOFT MATTER. - ISSN 1744-683X. - ELETTRONICO. - 12:(2016), pp. 9303-9313. [10.1039/c6sm01822j]

Structure of colloidal gels at intermediate concentrations: the role of competing interactions

Laurati M.
;
2016

Abstract

Colloidal gels formed by colloid–polymer mixtures with an intermediate volume fraction (fc E 0.4) are investigated by confocal microscopy. In addition, we have performed Monte Carlo simulations based on a simple effective pair potential that includes a short-range attractive contribution representing depletion interactions, and a longer-range repulsive contribution describing the electrostatic interactions due to the presence of residual charges. Despite neglecting non-equilibrium effects, experiments and simula- tions yield similar gel structures, characterised by, e.g., the pair, angular and bond distribution functions. We find that the structure hardly depends on the strength of the attraction if the electrostatic contribu- tion is fixed, but changes significantly if the electrostatic screening is changed. This delicate balance between attractions and repulsions, which we quantify by the second virial coefficient, also determines the location of the gelation boundary.
2016
12
9303
9313
Capellmann R.F.; Valadez-Perez N.E.; Simon B.; Egelhaaf S.U.; Laurati M.; Castaneda-Priego R.
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Utilizza questo identificatore per citare o creare un link a questa risorsa: https://hdl.handle.net/2158/1174685
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