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Immobilized layer

These effects can be illustrated more quantitatively. The drop in the magnitude of the potential of mica with increasing salt is illustrated in Fig. V-7 here yp is reduced in the immobile layer by ion adsorption and specific ion effects are evident. In Fig. V-8, the pH is potential determining and alters the electrophoretic mobility. Carbon blacks are industrially important materials having various acid-base surface impurities depending on their source and heat treatment. [Pg.190]

The hydrolysed surface of Ihe Si3N4 insulator functions as a pH-sensitive membrane [90, 105, 116, 179]. A penicillin-sensitive ISFET is based on this membrane that is covered by an immobilized layer of penicillinase, converting penicillin into the penicillanic acid anion with liberation of hydrogen ions [24]. Another version of pH-sensitive ISFETs has membrane gates made of TajOs [3] or of a suitable glass [39]. The latter ISFET with a gate made of alumino- or borosilicate glass is sensitive to sodium ions. Other ISFETs are sensitive to halide ions [22, 153, 178], [105, 115, 130] and Ca [90, 105]. [Pg.77]

Next, let us consider the application of Equation (21) to a particle migrating in an electric field. We recall from Chapter 4 that the layer of liquid immediately adjacent to a particle moves with the same velocity as the surface that is, whatever the relative velocity between the particle and the fluid may be some distance from the surface, it is zero at the surface. What is not clear is the actual distance from the surface at which the relative motion sets in between the immobilized layer and the mobile fluid. This boundary is known as the surface of shear. Although the precise location of the surface of shear is not known, it is presumably within a couple of molecular diameters of the actual particle surface for smooth particles. Ideas about adsorption from solution (e.g., Section 7.7) in general and about the Stern layer (Section 11.8) in particular give a molecular interpretation to the stationary layer and lend plausibility to the statement about its thickness. What is most important here is the realization that the surface of shear occurs well within the double layer, probably at a location roughly equivalent to the Stern surface. Rather than identify the Stern surface as the surface of shear, we define the potential at the surface of shear to be the zeta potential f. It is probably fairly close to the... [Pg.541]

Shichiri et al(ll) (Osaka University in Japan) has developed the micro needle type glucose sensor, which consisted of a hydrogen peroxide electrode and a GOX enzyme immobilized layer. The sensor was clinically used, but it had to be renewed after a few days because of a gradual decline in its output. [Pg.374]

The electrocatalytic oxidation of D-gluconic acid at an ubiquinine-mixed carbon paste electrode with an immobilized layer of D-gluconate dehydrogenase has been described.259... [Pg.231]

T. Ikeda, K. Miki, F. Fushimi, and M. Senda, Electrocatalytic oxidation of D-gluconate at a ubiquinone-mixed carbon paste electrode with an immobilized layer of D-gluconate dehydrogenase from bacterial membranes, Agric. Biol. Chem., 51 (1987) 747-754. [Pg.293]

The diagrams of the direct synthesis of alkyl- and arylchlorosilanes differ mostly in the construction of the contact apparatus. At present there are two basic types of contact apparatuses known stationary reactors, in which contact mass is in the immobile layer, and nonstationary reactors, in which contact mass is mobile. [Pg.54]

With large K values, that is low solubility of component i in a liquid food, the material transport through A can also be determined from the contribution of diffusion in L under conditions of thorough mixing. Van der Waals attractive forces between the package surface and the molecules of L in intimate contact with P lead to the formation of a thin but immobile layer in which the diffusion coefficient of i in L, DL, controls mass transport (the Nernst diffusion layer). [Pg.209]

Acetylcholineesterase A 350 pM diameter coherent imaging fiber coated on the distal surface with a planar layer of analyte-sensitive polymer that was thin enough not to affect the fiber s imaging capabilities. It was applied to a pH sensor array and an ACh biosensor array (each contain 6000 optical sensor). Fibers were coated with an immobilized layer of poly (hydroxyethylmethacrylate)-N-flurosceinylacrylamide and AChE-fluorescein isothiocyanate isomer poly (acryloamide-co-N-acryl oxysuccinimide), respectively. The response time of the pH sensor was 2 s for a 0.5 unit increase in pH. The biosensor had a detection limit of 35 pM ACh and a linear response in the range 0.1 mM. [90]... [Pg.41]

Acetylcholineesterase and choline oxidase A glassy C electrode surface was modified with osmium poly (vinyl-pyridine) redox polymer containing horseradish peroxidase (Os-gel-HRP) and then coated with a co-immobilized layer of AChE and ChO. A 22 pL pre-reactor, in which ChO and catalase were immobilized on beads in series, was used to remove choline. The variation in extracellular concentration of ACh released from rat hippocampal tissue culture by electrical stimulation was observed continuously with the online biosensor combined with a microcapillary sampling probe. Measurement of ACh and Ch was carried out by using a split disc C film dual electrode. [Pg.47]

Immobilized layer Glucose + FAD — Gluconolactone -I- FADH2 [2] FADH2 + 02 FAD + H2O2 [3]... [Pg.72]

Steric Hindrance. Another form of stabilization is relatively independent of ionic strength the oil droplets are prevented from making contact by simple steric hindrance. This may take two forms, either an immobilized water layer at the interface or a solid interfacial film. Emulsion stabilization by proteins, gums, and polyoxyethylene derivatives occurs by the first mechanism. Hydrophobic parts of the stabilizers adsorb at the oil surface, but adjacent large hydrophilic segments are hydrated and form an immobilized layer on the order of 10-100 nm thick (Figure 9). As mentioned, these hydrated segments frequently interact to cause flocculation, while coalescence of the oil drops themselves is prevented. Such emulsions are frequently used as carriers for oil-soluble flavors, essences, and colorants. [Pg.2214]

Note that the separation of the solution into two parts near a wall, that is, the immobile layer and the agitated homogeneous solution, is really simplistic since there is a continuous variation in the fluid velocity from the wall to the bulk [105]. Yet this dichotomous approximation is sufficient for most purposes and allows great simplifications in physicomathematical treatments of the transport problem. [Pg.64]

Summarizing, two conditions must be fulfilled in order to obtain from the simulations a confinement-induced and thickness-dependent distribution of the end-to-end distance for terminal subchains. First, a chain should be in contact with both interfaces. This happens only when the film thickness becomes comparable to the size of the chains and, obviously, explains why the confinement-induced mode does not exist in the bulk. Second, the interactions at the interfaces should be asymmetric One interface should immobilize the polymer chains, while the second one should only reflect them. This asymmetry could be induced by the nonequivalent preparation of the electrodes in the experiment While one interface is prepared by spin-coating, the other one is prepared by evaporation of aluminium on top of the polymer film (see Section II for details). A similar picture of asymmetry was found in studies on thin PS films, with a preparation procedure identical with ours. For thin PS films capped between two aluminum electrodes a three-layer model was proposed, in which, in addition to a middle-layer having bulk properties, a dead (immobilized) layer and a liquid-like layer were assumed to be present at the interfaces. [Pg.610]

Fig. 6.11. Typical packing structures in concentrated suspensions (a) simple network of chains (b) denser floes, cormected by chains (c) dense packing of spheres surroimded by a thick immobile layer of solvent or absorbed species (redrawn from Sormtag and Strenge [6]). Fig. 6.11. Typical packing structures in concentrated suspensions (a) simple network of chains (b) denser floes, cormected by chains (c) dense packing of spheres surroimded by a thick immobile layer of solvent or absorbed species (redrawn from Sormtag and Strenge [6]).
A common feature of electrokinetic phenomena is a relative motion of the charged surface and the volumetric phase of the solution. The charged surface is affected by the electric field forces, and the movement of such surfaces toward each other induces the electrical field. That is a question of slip plane between the double layer and a medium. The layer bounded by the plane at the distance d from surface (OHP) can be treated as immobile in the direction perpendicular to the surface, because the time of ion residence in the layer is relatively long. Mobilty of ions in the parallel direction to the interfacial surface should also be taken into account. However, it seems that the ions in the double layer and in the medium surrounding it constitute a rigid whole and that the layer from x = 0 to X = d is immobile also in the sense of resistance to the tangent force action. There is no reason why the boundary plane of the solution immobile layer should overlap accurately with the OHP plane. It can be as well placed deeply in the solution. The potential in the boundary plane of the solution immobile layer is called potential (. Strictly speaking it is not a potential of interface because it is created in the liquid phase. It can be considered as the difference of potentials between a point far from the surface (in the bulk solution) and that in the slip plane. [Pg.389]

Figure 2-10 Principles of RIfS A change in the optical thickness (a product of physical thickness and refractive index) of the immobilized layer due to binding will trigger a shift in the interference pattern. Figure 2-10 Principles of RIfS A change in the optical thickness (a product of physical thickness and refractive index) of the immobilized layer due to binding will trigger a shift in the interference pattern.
Shang et al. (1995) show that the work of adhesion between a silica filler surface and a polymer matrix is directly related to the dynamic viscosity and moduli. Additionally, at lower frequencies there is a greater influence of the work of adhesion. The influence is shown to be described well by an effective increase in interphase thickness due to the increase in the work of adhesion, such that polymer chains are effectively immobilized around the filler, and the friction between the immobilized layer and the polymer then governs the dynamic rheology. It was noted that the immobilized layer could be reduced in extent at higher frequencies. [Pg.360]

Usual enzyme electrodes are assemblies of several membranes placed one on top of the other. The sensitive enzyme membrane is mostly mechanically stabilized by a thin, enzyme-free dialysis membrane. Whether this arrangement is taken into account or neglected in favor of simplicity affects the quality of the model to a major extent. In sensors using more than one enzyme, the enzymes may be coimmobilized in one membrane or applied as immobilized layers in separate, sandwiched membranes. The respective models are different. [Pg.67]

For particles in oil, b decreases with 0 and also with 4>. In fact, the controlling parameter is o4>. Generally, a plot of 1/b versus o4) will produce a single curve in which b may drop from 5 at low stress to 2 at high stress where the immobilized layer is largely sloughed off. [Pg.752]


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