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Particle surface coverage, effect parameters

However, in subsequent studies [23-25,88-90] it was demonstrated that in reality the particle deposition is not a purely geometric effect, and the maximum surface coverage depends on several parameters, such as transport of particles to the surface, external forces, particle-surface and particle-particle interactions such as repulsive electrostatic forces [25], polydispersity of the particles [89], and ionic strength of the colloidal solution [23,88,90]. Using different kinds of particles and substrates, values of the maximum surface coverage varied by as much as a factor of 10 between the different studies. [Pg.229]

In the case of monolayer adsorption, a limiting adsorption value exists that is attained when the surface is covered completely by particles of a given substance (i.e., at full monolayer coverage). The limiting adsorption value depends on the effective surface area Sj taken up by one particle 1/5. This parameter characterizes the number of sites that can be occupied by adsorbed particles on a given surface. [Pg.156]

Fig. 4.10. Sketch of adsorption of polydisperse particles at (a) low and (b) high salt concentrations. Dotted lines show the effective particle radius (or interaction distance), (c) Surface coverage of the polystyrene particles versus na ( a is a dimensionless screening parameter, where k is the inverse Debye length and a the particle diameter). The more polydisperse particles (41 versus 107nm) have a slightly increased coverage at high na. Solid curves are approximations derived from the effective hard sphere model (see [89] for further details)... Fig. 4.10. Sketch of adsorption of polydisperse particles at (a) low and (b) high salt concentrations. Dotted lines show the effective particle radius (or interaction distance), (c) Surface coverage of the polystyrene particles versus na ( a is a dimensionless screening parameter, where k is the inverse Debye length and a the particle diameter). The more polydisperse particles (41 versus 107nm) have a slightly increased coverage at high na. Solid curves are approximations derived from the effective hard sphere model (see [89] for further details)...
Table 1 Averaged fitting results obtained for the structure parameters along the OC segment of the isotherms. Distance between nearest neighbours, D, particle diameter, d, surface coverage, y, immersion depth, k, all from the gradient-layer model. Effective refractive index, efr, diameter, Jhom both from the uniform-layer method. Diameter obtained from the transmission electron microscope images, 5 tem ... Table 1 Averaged fitting results obtained for the structure parameters along the OC segment of the isotherms. Distance between nearest neighbours, D, particle diameter, d, surface coverage, y, immersion depth, k, all from the gradient-layer model. Effective refractive index, efr, diameter, Jhom both from the uniform-layer method. Diameter obtained from the transmission electron microscope images, 5 tem ...
Fig. 7 Correlation among the layer parameters (immersion depth, h, particle diameter, d, distance between the centers of nearest neighbours, D, surface coverage, y), Wgfr and the surface pressure, II a immersion of particles versus surface pressure b surface coverage versus surface pressure c the change of the effective refractive index with compression and d correlation between the effective refractive index and the rate of silica in the layer that is submerged in water. Hydrophobic particles closed circles), hydrophilic particles open circles)... Fig. 7 Correlation among the layer parameters (immersion depth, h, particle diameter, d, distance between the centers of nearest neighbours, D, surface coverage, y), Wgfr and the surface pressure, II a immersion of particles versus surface pressure b surface coverage versus surface pressure c the change of the effective refractive index with compression and d correlation between the effective refractive index and the rate of silica in the layer that is submerged in water. Hydrophobic particles closed circles), hydrophilic particles open circles)...
As aforementioned, there is a trade-off between (1) the adsorbed amounts of the reactants and the surface coverage in hydroxyl groups both of which are considered to be favorable factors for the photocatalytic rates (these factors increase with the surface area and hence with decreasing particle sizes) and (2) the unfavorable recombination rate of the photoproduced charges at the structural irregularities whose density should be higher on smaller particles [84]. Also, the effect of the actual particle size on the absorption and scattering of useful photons is a parameter to be taken into account [8] (see Sect. 10.2.1). In practice, appropriate trials are required. [Pg.342]

For the linearly adsorbed CO, the shift of the C-O vibrational frequency upon carrier doping may be related to three factors (1) effects of the surface electronic states of the Rh crystallites (2) Rh particle size (due to the Rh-Rh bond disruption) and (3) changes of CO coverage. In order to eliminate any shift due to factors other than electronic parameters, the position of the linear CO bands on the doped and the undoped catalysts obtained at small and equal CO coverage are compared. Low 0co was obtained by careful control of CO exposure to the fresh sample. Figure 6 shows the spectral features of CO (0co = 0.08-0.09) adsorbed on the doped (x = 0.67 at.%) and the undoped catalysts, following CO exposure at 300 K. The linear CO band is... [Pg.776]


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See also in sourсe #XX -- [ Pg.405 , Pg.406 ]




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