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Charge of surface

Adsorption related charging of surface naturally affects the value of the thermoelectron work function of semiconductor [4, 92]. According to definition the thermoelectron work function is equal to the difference in energy of a free (on the vacuum level) electron and electron in the volume of the solid state having the Fermi energy (see Fig. 1.5). In this case the calculation of adsorption change in the work function Aiqp) in... [Pg.38]

Fig. 6-99. An interfacial electric double layer on semiconductor electrodes a = charge of surface states 0.1 = interfadal charge of adsorbed ions IHP = inner Helmholtz plane. Fig. 6-99. An interfacial electric double layer on semiconductor electrodes a = charge of surface states 0.1 = interfadal charge of adsorbed ions IHP = inner Helmholtz plane.
The interfacial excess charge of semiconductor electrodes consists of the space charge osc on the semiconductor side the charge of surface states o the charge Oh of interfacial hydroxyl groups the charge Oms of adsorbed ions in the compact... [Pg.184]

For simple semiconductor electrodes on which the charge of surface states and the charge of adsorbed ions are zero or remain constant, the flat band potential is obtained from Eqn. 5-84 to give Eqn. 5-87 ... [Pg.185]

Fig. 6-53. Interfadal charges, electron levels and electrostatic potential profile across an electric double layer with contact adsorption of dehydrated ions on semiconductor electrodes ogc = space charge o = charge of surface states = ionic charge due to contact adsorption dsc = thickness of space charge layer da = thickness of compact la3rer. Fig. 6-53. Interfadal charges, electron levels and electrostatic potential profile across an electric double layer with contact adsorption of dehydrated ions on semiconductor electrodes ogc = space charge o = charge of surface states = ionic charge due to contact adsorption dsc = thickness of space charge layer da = thickness of compact la3rer.
This equivalence between the charge of surface-bound molecules and the current of solution soluble ones is due to two main reasons first, in an electro-active monolayer the normalized charge is proportional to the difference between the total and reactant surface excesses ((QP/QP) oc (/> — To)), and in electrochemical systems under mass transport control, the voltammetric normalized current is proportional to the difference between the bulk and surface concentrations ((///djC) oc (c 0 — Cq) [49]. Second, a reversible diffusionless system fulfills the conditions (6.107) and (6.110) and the same conditions must be fulfilled by the concentrations cQ and cR when the process takes place under mass transport control (see Eqs. (2.150) and (2.151)) when the diffusion coefficients of both species are equal. [Pg.422]

Physical Particle size and size distribution True density Bulk and tapped densities Surface area Electric charge of surface Stability of solid state Porosity Hygroscopicity Compactibility Intrinsic dissolution... [Pg.170]

The sheaf of the C 2 vs. E straight lines generally evidences some slow process proceeding either on the semiconductor surface (e.g. adsorption, charging of surface states) or in the space charge region (e.g. the deep donor or acceptor ionization mentioned above). [Pg.235]

In the full-cell process, the wood in the cylinder first is subjected to a vacuum of not less than 22 in. Hg for 15-60 min, to remove as much air as possible from the wood. The cylinder then is filled with hot treating liquid without admitting air. The maximum temperature for creosote and its solutions is 210°F, and for water-borne preservatives it is 120-150°F, depending upon the preservative. Then the liquid is placed under a pressure of 125-200 psi, and the temperature and pressure are maintained for the desired length of time, usually several hours. After the liquid is drawn from the cylinder, a short vacuum is applied to free the charge of surface-dripping preservative. [Pg.1270]

If a spherical drop of water carries an electric charge (such as a drop in a thunder-cloud), this resides in the surface, and a charge of surface density k causes a hydrostatic tension 2jtk per cm., acting along the outward-drawn normal to the surface and tending to explode the drop. ... [Pg.375]

Deviations from straight lines in Mott-Schottky plots can be attributed to the influence of potential-dependent charging of surface or bulk states. This interpretation is supported by analytic calculations of the contribution of defects to the space charge as a function of applied potential. In principle, the... [Pg.230]

At first we observed XRD to confirm whether any aggregation was caused by Li addition or not. No detectable growth of metal particles was observed upon Lidoping. We also carried out XPS measurements to observe modification of charge of surface Rh species by Li addition, which might verify reactivity. However, Rh... [Pg.458]

S. Chen R. W. Murray, Electrochemical Quantized Capacitance Charging of Surface Ensembles of Gold Nanoparticles. J. Phys. Chem. B 1999, 103, 9996-10000. [Pg.643]

Chen, S.W. and Murray, R.W. (1999) Electrochemical quantized capacitance charging of surface ensembles of gold nanopartides. Journal of Physical Chemistry B, 103, 9996-10000. [Pg.141]

Ray, K.C. and Sen, P.K., Correlation of zero points of charge of solid oxides and hydroxides with partial charge of surface oxygen atom, Indian J. Chem., 12, 170, 1974. [Pg.1050]

The factors which lead to the formation of an electrical double layer are rather general. First, charges flow across the interface when a thermodynamic equilibrium is established between the phases in contact second, it is charging processes, which are not generally related to charge transfer across the interface—for example, charging of surface states (see below), certain types of adsorption, etc. [Pg.201]

The correction factor for positive and negative ions will have opposite signs and will cancel. However, although individual surface complexation reactions (e.g., Equations (7.12) - (7.14)) are charge balanced, there is often a net change in charge of surface species (sites). For example, in Equation (7.12), Az = — 1. This is the number of charges that must be transferred from the solution to the surface, or vice versa. The ArG° of the surface complexation reaction will therefore have a correction factor of A or... [Pg.141]

Fig. 9a-c. Shift of energy bands of WSe2 in presence of different redox agents. A different kinetics (surface position of quasi Fermi-level), different surface states as well as a different charging of surface states can be involved... [Pg.141]

The effects of the difference in hydrophobicity/hydrophilicity on water structure was captured in an elegant thought, or rather computer, experiment where the partial charges of surface atoms were tuned from zero to the normal charge distribution. When the partial charge is zero q = 0), then the surface behaves like an apolar/ hydrophobic surface. On the other hand, when the charge distribution is normal iq = 1), the surface is hydrophilic. In both scenarios, the water dynamics in the adjacent layer slows down but for quite different reasons [5]. We will discuss this important result in more detail. [Pg.204]

The newly developed approach for ion adsorption treats the charge of surface... [Pg.79]

The water film adsorbed on the surface and neutralizing the charges of surface atoms provides the surface energy lowering of AF. The vapour pressure over the solid phase can be calculated from the adsorption isotherm ... [Pg.329]


See other pages where Charge of surface is mentioned: [Pg.204]    [Pg.227]    [Pg.315]    [Pg.440]    [Pg.326]    [Pg.320]    [Pg.264]    [Pg.301]    [Pg.261]    [Pg.55]    [Pg.410]    [Pg.239]    [Pg.310]    [Pg.813]    [Pg.543]    [Pg.640]    [Pg.722]    [Pg.46]    [Pg.159]    [Pg.161]    [Pg.59]    [Pg.158]    [Pg.56]    [Pg.366]    [Pg.500]    [Pg.255]   
See also in sourсe #XX -- [ Pg.175 , Pg.177 ]




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