1995
DOI: 10.1039/fd9950100185
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Gelation of proteins from milk

Abstract: We give a quantitative treatment of the destabilization of three types of milk protein dispersions. For this we consider the proteins as adhesive-hardsphere bio-colloids. If the attractive interactions become strong enough the system passes the percolation threshold and gels. Macroscopic properties of these gels are studied by measuring viscoelasticity and permeability coefficients. These coeficients are related to structural (fractal) properties of the gels which were measured using scattering and confocal sc… Show more

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Cited by 56 publications
(31 citation statements)
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“…One way to include this attractive part is the Baxter model (Figure 1.2), (Baxter, 1968) commonly known as the "adhesive hard sphere model". It describes the adhesiveness by using a parameter t, which is related to the depth of the attractive well in the interaction potential while its width is regarded to be infinitely small (de Kruif et al, 1995;Mezzenga & Fischer, 2013). Using the Baxter model it is possible to derive the following expression for the osmotic pressure (Parker, Noel, Brownsey, Laos, & Ring, 2005;Prinsen & Odijk, 2004):…”
Section: Theorymentioning
confidence: 99%
“…One way to include this attractive part is the Baxter model (Figure 1.2), (Baxter, 1968) commonly known as the "adhesive hard sphere model". It describes the adhesiveness by using a parameter t, which is related to the depth of the attractive well in the interaction potential while its width is regarded to be infinitely small (de Kruif et al, 1995;Mezzenga & Fischer, 2013). Using the Baxter model it is possible to derive the following expression for the osmotic pressure (Parker, Noel, Brownsey, Laos, & Ring, 2005;Prinsen & Odijk, 2004):…”
Section: Theorymentioning
confidence: 99%
“…This model has been applied successfully to various systems having short-ranged attractive forces, including sterically stabilized dispersions (31), surfactant-based microemulsions (32), particles flocculated/gelled by bridging polymers (33,34), aggregating casein micelles (11,35), and flocculated caseincoated emulsion droplets (36). The sticky hard-sphere system has a critical temperature defined by τ c = 0.098 and a critical volume fraction φ c = 0.12.…”
Section: Reversible Aggregation and Gelationmentioning
confidence: 99%
“…Strong disulfide bonds can form between the protein molecules. The denatured proteins tend to aggregate even at low concentrations to form small particles (nanometer scale) (31)(32)(33)(34).…”
Section: Resultsmentioning
confidence: 99%