Please use this identifier to cite or link to this item: http://www.repository.rmutt.ac.th/xmlui/handle/123456789/444
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dc.contributor.authorParhi, Purnendu
dc.contributor.authorGolas, Avantika
dc.contributor.authorBarnthip, Naris
dc.contributor.authorNoh, Hyeran
dc.contributor.authorVogler, Erwin A.
dc.date.accessioned2012-03-06T05:39:08Z
dc.date.accessioned2020-09-24T04:56:32Z-
dc.date.available2012-03-06T05:39:08Z
dc.date.available2020-09-24T04:56:32Z-
dc.date.issued2009-12
dc.identifier.citationfrom Web of Scienceen_US
dc.identifier.issn0142-9612
dc.identifier.urihttp://www.repository.rmutt.ac.th/dspace/handle/123456789/444-
dc.descriptionVolumetric interpretation of protein adsorption: Capacity scaling with adsorbate molecular weight and adsorbent surface energy / http://isiknowledge.comen_US
dc.description.abstractSilanized-glass-particle adsorbent capacities are extracted from adsorption isotherms of human serum albumin (HSA, 66 kDa), immunoglobulin G (IgG, 160 kDa), fibrinogen (Fib, 341 kDa), and immunoglobulin M (IgM, 1000 kDa) for adsorbent surface energies sampling the observable range of water wettability. Adsorbent capacity expressed as either mass-or-moles per-unit-adsorbent-area increases with protein molecular weight (MW) in a manner that is quantitatively inconsistent with the idea that proteins adsorb as a monolayer at the solution-material interface in any physically-realizable configuration or state of denaturation. Capacity decreases monotonically with increasing adsorbent hydrophilicity to the limit-of-detection (LOD) near tau degrees = 30 dyne/cm (theta similar to 65 degrees) for all protein/surface combinations studied (where tau degrees gamma(l nu)degrees cos theta is the buffer advancing contact angle). Experimental evidence thus shows that adsorbent capacity depends on both adsorbent surface energy and adsorbate size. Comparison of theory to experiment implies that proteins do not adsorb onto a two-dimensional (2D) inter-facial plane as frequently depicted in the literature but rather partition from solution into a three-dimensional (3D) interphase region that separates the physical surface from bulk solution. This interphase has a finite volume related to the dimensions of hydrated protein in the adsorbed state (defining "layer" thickness). The interphase can be comprised of a number of adsorbed-protein layers depending on the solution concentration in which adsorbent is immersed, molecular volume of the adsorbing protein (proportional to MW), and adsorbent hydrophilicity. Multilayer adsorption accounts for adsorbent capacity over-and-above monolayer and is inconsistent with the idea that protein adsorbs to surfaces primarily through protein/surface interactions because proteins within second (or higher-order) layers are too distant from the adsorbent surface to be held surface bound by interaction forces in close proximity. Overall, results are consistent with the idea that protein adsorption is primarily controlled by water/surface interactions. (C) 2009 Elsevier Ltd. All rights reserved.en_US
dc.language.isoenen_US
dc.publisherELSEVIER SCI LTD, THE BOULEVARD, LANGFORD LANE, KIDLINGTON, OXFORD OX5 1GB, OXON, ENGLANDen_US
dc.subjectRANDOM SEQUENTIAL ADSORPTIONen_US
dc.subjectSCALED INTERFACIAL ACTIVITYen_US
dc.subjectDEPENDENT CONTACT ANGLESen_US
dc.subjectSOLID LIQUID ADSORPTION; ATOMIC-FORCE MICROSCOPYen_US
dc.subjectSERUM-ALBUMINen_US
dc.subjectBLOOD-PLASMAen_US
dc.subjectVAPOR INTERFACEen_US
dc.subjectADHESION FORCESen_US
dc.subjectAQUEOUS-BUFFERen_US
dc.titleVolumetric interpretation of protein adsorption: Capacity scaling with adsorbate molecular weight and adsorbent surface energyen_US
dc.typeArticleen_US
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