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Barrier to adsorption

Another possibility that could explain the effect of illumination is a change in the electric double layer surrounding the CdSe particles, either adsorbed on the substrate or in the solution, which could lower a potential barrier to adsorption and coalescence, as suggested previously for film formation from Se colloids under illumination [93]. Partial coalescence would reduce the blue spectral shift due to size quantization. However, the spectral shape is not expected to undergo a fundamental change in this case. The photoelectrochemical explanation therefore appears more reasonable. [Pg.176]

Once the interface is partially saturated with adsorbed solute molecules, then the rate of adsorption falls below the rate of diffusion, suggesting an energy barrier to adsorption. [Pg.13]

It is well-known that protein adsorption tends to be at a maximum at the isoelectric point because the protein has zero net charge. Under such conditions, electrostatic barriers to adsorption are minimized. [Pg.57]

The film diffusion process assumes that reactive surface groups are exposed directly to the aqueous-solution phase and that the transport barrier to adsorption involves only the healing of a uniform concentration gradient across a quiescent adsorbent surface boundary layer. If instead the adsorbent exhibits significant microporosity at its periphery, such that aqueous solution can effectively enter and adsorptives must therefore traverse sinuous microgrottos in order to reach reactive adsorbent surface sites, then the transport control of adsorption involves intraparticle diffusion.3538 A simple mathematical description of this process based on the Fick rate law can be developed by generalizing Eq. 4.62 to the partial differential expression36... [Pg.169]

Figure 8 Relationship between the width of the barrier to adsorption and the resulting desorption distribution (T = 600 K). As the sticking function (a) is broadened the energy release (b) decreases but the distribution retains a pronounced tail to high energy. Figure 8 Relationship between the width of the barrier to adsorption and the resulting desorption distribution (T = 600 K). As the sticking function (a) is broadened the energy release (b) decreases but the distribution retains a pronounced tail to high energy.
The sticking functions predicted by detailed balance on the basis of these desorption distributions are shown in Fig. 21 and predict that S E) increases exponentially with energy before starting to saturate near 2 eV. This provides an experimental estimate of 2 eV for the barrier to adsorption on Ru(0 001), which is consistent with the DFT calculations [103]. This interpretation of the desorption results predicts that dissociation will be highly activated with S < 10-8 at low energy, consistent with the very low S... [Pg.165]

Only a few kinetic studies of the rate of sulfur adsorption on metals have been made. They reveal that rates of adsorption of H2S on metals are generally very rapid, the high sticking probability suggesting no barrier to adsorption and dissociation until saturation is approached. In the case of Pt and Cu (83, 92), two adsorption regimes are observed (1) at 0 < 0.25-0.3, the adsorption of sulfur occurs with a high sticking coefficient ( 1.0) and... [Pg.153]

Before a protein molecule can adsorb and exert its influence at a phase boundary or take part in an interfacial reaction, it must arrive at the interface by a diffusion process. If we assume there is no barrier to adsorption other than diffusion, simple diffusion theory may be applied to predict the rate of adsorption. Under these conditions, after formation of a clean interface, all the molecules in the immediate vicinity will be rapidly adsorbed. The protein concentration in a sublayer, adjacent to the interface.and of several molecular diameters in thickness, will thus be depleted to zero. A diffusion process then proceeds from the bulk solution to the sublayer. The rate of adsorption, dn/dt, will be simply equal to the rate of this diffusion step given by classical diffusion theory (Crank, 1956) as... [Pg.286]

When a protein adsorbs from a solution in which the pH is close to its isoelectric point, the rate of adsorption at mobile interfaces is controlled by the rate of diffusion to the interface and the interfacial pressure barrier. However, when the protein molecule takes on a net electrical charge, an additional barrier to adsorption appears, owing to the electrical potential set up at the interface by the adsorbed protein. [Pg.290]

Transfer of surfactant molecules from the subsurface to the adsorption layer the rate of transfer is determined by the height of the kinetic barrier to adsorption... [Pg.162]

It must be noted that this is a schematic diagram where the abscissa is not a linear distance scale instead it represents the trajectory pathway of an incoming molecule to a surface. Dissociative adsorption can occur from a weakly held molecular state if the net barrier to adsorption is low (precursor mediated) but is of low probability if it is high. Then it is only the hot molecules of the Maxwell Boltzmann distribution of velocities (fig. 9) which can dissociate and they do this by direct passage over the energy barrier (direct activated). The rate of dissociation from a precursor state can be written as follows for the simple case in fig. 9,... [Pg.298]

Fig. 22. The effect of sulphur poisoning on the speed profile of molecules detected by their time of flight. In the absence of S, Lhe distribution is essentially Maxwellian showing desorption with no net adsorption activation barrier, while after poisoning the speed distribution is sharp and indicative of fast molecules desorbing over a net activation barrier to adsorption. From Comsa et al. (19S0). Fig. 22. The effect of sulphur poisoning on the speed profile of molecules detected by their time of flight. In the absence of S, Lhe distribution is essentially Maxwellian showing desorption with no net adsorption activation barrier, while after poisoning the speed distribution is sharp and indicative of fast molecules desorbing over a net activation barrier to adsorption. From Comsa et al. (19S0).
The Marangoni effect is signihcant only in dilute solution and within a limited concentration range. The amount of solute adsorbed at a new surface in the absence of stirring or an energy barrier to adsorption is given by (Ward, 1946)... [Pg.279]

Calculate the time it would take for the surface concentration to reach a value of 2 x 10 10 mol/cm2 from a 1 x 10 2 M solution of surfactant in the absence of stirring or an energy barrier to adsorption. Assume the bulk diffusion constant of the surfactant to be 2 x 106 cm2/s. [Pg.302]

The simulations can also provide mechanistic insight into the adsorption process. In the case of Li+ it was shown that the free energy barrier is associated with the temporary loss of hydration shell molecules, while the increase of 1 hydration number is indicative of a mechanism where the steric barrier to adsorption by the adsorbate water layer is most important. [Pg.53]

Kolasinski et al. [70] found that there was no translational energy in excess of that expected at equilibrium, while Park et al. [69] found a higher ratio of normal translational energy than expected at equilibrium. These results appear to contradict each other, though this is not a strict logical necessity. Within their simplest interpretations, both experiments agree that any barrier to adsorption in the normal coordinate is at most a few kilocalories per mole. [Pg.26]

These predictions are consistent with the experimental value of 58 kcal/ mol for the activation barrier to desorption, but it permits only a small barrier for the reverse adsorption reaction. Nachtigall et al. [75] pointed out that if there is a substantial activation barrier to adsorption, these calculations could not be consistent with desorption from a prepaired state. They suggested that a more complex, multistep mechanism might be responsible for desorption. For example, they drew an analogy with gas-phase elimination of H2 from disilane, in which the 1,1-elimination mechanism has a lower activation barrier than the 1,2-elimination [75]. They suggested that desorption may occur by a 1,2-hydrogen shift (to form a dihydride) followed by 1,1-elimination (desorption of the dihydride). This speculation was supported... [Pg.33]

The defect-mediated mechanisms have desorption from the dihydride as a final step. Consequently, they all predict that the transition state for desorption is only a few (3-5) kilocalories per mole above the product state. This is consistent with the observation that product H2 has little excess energy. On the other hand, the low excess energy of the transition state over the desorbed state means that the defect-mediated mechanisms have corresponding low barriers to adsorption. At the time these mechanisms were proposed, there were no measurements of the activation energy to adsorption. If the more recent evidence [41, 73] that adsorption has a high activation barrier is confirmed, these models must be ruled out or at least substantially modified. [Pg.44]


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See also in sourсe #XX -- [ Pg.314 ]




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Adsorption barriers

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