1998
DOI: 10.1006/jcis.1998.5846
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Effect of Ethanol on the Structure and Properties of β-Casein Adsorption Layers at the Air/Buffer Interface

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Cited by 37 publications
(42 citation statements)
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“…The surface compression moduli expressed as a function of π are clearly not monotonic, and in the case of c‐Fos it exhibits two maxima (Inset in Figure 3), supporting the concept that the proteins we are dealing with are flexible 48. Moreover, if we assume that, despite the obvious differences between the K vs. π and ε vs. π dependences, the Flory exponent γ taken from the slopes of K vs. π curves relates to the molecular arrangement at the interface,49 the slope values of 5 and 1 for c‐Fos in the lineal region before the first and the second maximum respectively, mean that the surface behavior is dominated by the hydrophobic portions of the protein along the interface at low surface pressure (dilute regime), and by the hydrophilic portions forming a network in the bulk just below the interface at higher pressures (semidilute regime) 49. The fact that Fra‐1 and c‐Jun do not present a second maximum implies that these two proteins do not transition to a network at high packing; this translates in a little cooperative molecular reordering at intermediate surface pressures.…”
Section: Resultsmentioning
confidence: 62%
“…The surface compression moduli expressed as a function of π are clearly not monotonic, and in the case of c‐Fos it exhibits two maxima (Inset in Figure 3), supporting the concept that the proteins we are dealing with are flexible 48. Moreover, if we assume that, despite the obvious differences between the K vs. π and ε vs. π dependences, the Flory exponent γ taken from the slopes of K vs. π curves relates to the molecular arrangement at the interface,49 the slope values of 5 and 1 for c‐Fos in the lineal region before the first and the second maximum respectively, mean that the surface behavior is dominated by the hydrophobic portions of the protein along the interface at low surface pressure (dilute regime), and by the hydrophilic portions forming a network in the bulk just below the interface at higher pressures (semidilute regime) 49. The fact that Fra‐1 and c‐Jun do not present a second maximum implies that these two proteins do not transition to a network at high packing; this translates in a little cooperative molecular reordering at intermediate surface pressures.…”
Section: Resultsmentioning
confidence: 62%
“…The study of the rheological parameters of adsorption layers of proteins and synthetic polyelectrolytes, in particular, dilatational characteristics, demonstrates an unusual behavior of the elastic modulus (to be exact, viscoelastic modulus) E defined by the relation (26) (A is the surface area) as depending on the bulk concentration, surface pressure, or protein adsorption [36,[54][55][56][57][58][59][60][61][62][63]. In the Maxwell model, the modulus E is expressed as a complex number comprising real (elasticity) and imaginary (viscosity) components: (27) In the case of diffusion-limited adsorption and in the absence of other relaxation processes in the surface layer, the real and imaginary components of the complex elastic modulus are expressed as functions of the frequency f of the surface perturbations and the surfactant (or protein) concentration as follows [59,61]: (28) where ζ = , E 0 = dΠ/dlnΓ is the limiting high-frequency (Gibbs) elasticity, and ω D = D(dΓ/dc) -2 is the characteristic frequency of the diffusion relaxation.…”
Section: Elastic Modulus and Limiting Elasticity Of A Surface Layermentioning
confidence: 99%
“…Experimental data [36,[54][55][56][57][58][59][60][61] testify that the E value for globular proteins is substantially larger than that for flexible-chain proteins and monotonically increases to a certain limiting value with the surface pressure or adsorption. At the same time, for flexiblechain proteins, E is not only smaller by several times than for globular proteins, but its dependences on the surface pressure or adsorption pass through a maximum.…”
Section: Elastic Modulus and Limiting Elasticity Of A Surface Layermentioning
confidence: 99%
“…Surface tension was measured using a pendant drop tensiometer from IT Concept, Longessaigne, France (Labourdenne et al ., 1994; Puff et al ., 1998; Péron et al ., 2000, 2001). An air bubble was formed in the liquid at the tip of the needle of a syringe whose plunger position was driven by a computer.…”
Section: Experimental Samples and Set‐upsmentioning
confidence: 99%