1998
DOI: 10.1016/s0927-7757(98)00512-3
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Predicting equilibrium constants for ion exchange of proteins — a colloid science approach

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Cited by 14 publications
(10 citation statements)
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“…The interaction between protein and adsorbent could be treated as a colloidal interaction, which is well characterized by zeta potential (26–28). The zeta potential depends on the surface charge of colloidal particle and environmental properties, such as pH and ionic strength.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…The interaction between protein and adsorbent could be treated as a colloidal interaction, which is well characterized by zeta potential (26–28). The zeta potential depends on the surface charge of colloidal particle and environmental properties, such as pH and ionic strength.…”
Section: Resultsmentioning
confidence: 99%
“…The increase of ionic strength leads to a decrease of the electrostatic interactions or, in other words, the decrease of the equilibrium constant in the SMA model. With the other theoretical framework different from the SMA model, Bowen et al also found that in their model the ion exchange equilibrium constant of BSA binding to QA52 ion exchanger decreased with increasing ionic strength (26).…”
Section: Resultsmentioning
confidence: 99%
“…In this case, one cannot simply use the results established by considering the membrane as a flat homogeneous plane (such as the one giving the DLVO potential for a sphere-infinite plane geometry, for instance) and a more realistic approach has to be developed. This significantly complicates any calculation of particle-membrane interactions [43][44][45][46]. Also, the description of the particle convective motion towards the membrane is also made much more complex when working at pore scale, as the hydrodynamic interactions between the particle and the membrane have to be accounted for.…”
Section: Towards a Pore Scale Approachmentioning
confidence: 99%
“…Several models have been considered to describe adsorption of charged species at charged interfaces based on the Poisson-Boltzmann equation. The simplified case corresponding to adsorption of spheres with an evenly distributed net-charge has been treated, [9][10][11][12][13][14][15] and other approaches include structural features and orientation of the macromolecule. [16][17][18] An important difference is the fact that the later approach introduces some anisotropy in the charge distribution on the protein, as it has long been recognized that protein adsorption at charged interfaces cannot be satisfactorily explained by the overall net-charge, [19][20][21] due to the asymmetrical distribution of groups of different charge on the protein surface.…”
Section: ' Introductionmentioning
confidence: 99%