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Electroneutral substances that are less polar than the solvent and also those that exhibit a tendency to interact chemically with the electrode surface, e.g. substances containing sulphur (thiourea, etc.), are adsorbed on the electrode. During adsorption, solvent molecules in the compact layer are replaced by molecules of the adsorbed substance, called surface-active substance (surfactant).t The effect of adsorption on the individual electrocapillary terms can best be expressed in terms of the difference of these quantities for the original (base) electrolyte and for the same electrolyte in the presence of surfactants. Figure 4.7 schematically depicts this dependence for the interfacial tension, surface electrode charge and differential capacity and also the dependence of the surface excess on the potential. It can be seen that, at sufficiently positive or negative potentials, the surfactant is completely desorbed from the electrode. The strong electric field leads to replacement of the less polar particles of the surface-active substance by polar solvent molecules. The desorption potentials are characterized by sharp peaks on the differential capacity curves. [Pg.235]

It should be emphasized that the electrochemical carbonization proceeds, in contrast to all other common carbonization reactions (pyrolysis), already at the room temperature. This fact elucidates various surprising physicochemical properties of electrochemical carbon, such as extreme chemical reactivity and adsorption capacity, time-dependent electronic conductivity and optical spectra, as well as its very peculiar structure which actually matches the structure of the starting fluorocarbon chain. The electrochemical carbon is, therefore, obtained primarily in the form of linear polymeric carbon chains (polycumulene, polyyne), generally termed carbyne. This can be schematically depicted by the reaction ... [Pg.327]

Figure 5. Schematic depiction of a self-encoded bead array. A mixture of three sensor types fills the fiber tip wells randomly. The sensors are identified by their characteristic responses to a test vapor pulse. Reprinted with permission from ref. 9b. Copyright 1999 American Chemical Society. Figure 5. Schematic depiction of a self-encoded bead array. A mixture of three sensor types fills the fiber tip wells randomly. The sensors are identified by their characteristic responses to a test vapor pulse. Reprinted with permission from ref. 9b. Copyright 1999 American Chemical Society.
Schematic depiction of the structural evolution of polymer electrolyte membranes. The primary chemical structure of the Nafion-type ionomer on the left with hydrophobic backbone, side chains, and acid head groups evolves into polymeric aggregates with complex interfacial structure (middle). Randomly interconnected phases of these aggregates and water-filled voids between them form the heterogeneous membrane morphology at the macroscopic scale (right). Schematic depiction of the structural evolution of polymer electrolyte membranes. The primary chemical structure of the Nafion-type ionomer on the left with hydrophobic backbone, side chains, and acid head groups evolves into polymeric aggregates with complex interfacial structure (middle). Randomly interconnected phases of these aggregates and water-filled voids between them form the heterogeneous membrane morphology at the macroscopic scale (right).
The pyroxenes are chemically complex but common rock-forming minerals. They resemble the amphiboles in many ways, but are actually single-chain silicates. The tetrahedral basic unit of the pyroxenes, [(Al,Si)20g] , was schematically depicted in Fig. 2.1C. The general formula for the group is Ai (B, C)i+ TjOfi, where A = Ca" Fe Li+, Mg "", Na-" B = Mg ", Fe Mn" Sc+ C = Fe A Cr" Ti " and T = Si Al+l Within the group are several mineral series and several species that often occur in acicular or fibrous forms. One species that occurs in fibrous form is jadeite, [Na(Al,Fe )Si206], a relatively familiar name because of the popularity of this material with Oriental sculptors. [Pg.48]

The significant intrinsic limitation of SEC is the dependence of retention volumes of polymer species on their molecular sizes in solution and thus only indirectly on their molar masses. As known (Sections 16.2.2 and 16.3.2), the size of macromolecnles dissolved in certain solvent depends not only on their molar masses but also on their chemical structure and physical architecture. Consequently, the Vr values of polymer species directly reflect their molar masses only for linear homopolymers and this holds only in absence of side effects within SEC column (Sections 16.4.1 and 16.4.2). In other words, macromolecnles of different molar masses, compositions and architectures may co-elute and in that case the molar mass values directly calculated from the SEC chromatograms would be wrong. This is schematically depicted in Figure 16.10. The problem of simultaneous effects of two or more molecular characteristics on the retention volumes of complex polymer systems is further amplifled by the detection problems (Section 16.9.1) the detector response may not reflect the actual sample concentration. This is the reason why the molar masses of complex polymers directly determined by SEC are only semi-quantitative, reflecting the tendencies rather than the absolute values. To obtain the quantitative molar mass data of complex polymer systems, the coupled (Section 16.5) and two (or multi-) dimensional (Section 16.7) polymer HPLC techniques must be engaged. [Pg.475]

Figure 6.1 Schematic depiction of Gibbs equilibration for three driving forces (a) thermal (T difference), (b) electrical ( emf difference), (c) chemical (pq difference), showing the transported quantity Xt and available work RffXi for each driving field / /. Figure 6.1 Schematic depiction of Gibbs equilibration for three driving forces (a) thermal (T difference), (b) electrical ( emf difference), (c) chemical (pq difference), showing the transported quantity Xt and available work RffXi for each driving field / /.
Figure 13.2 Schematic depiction of chemical diffusion (arrows) induced by chemical potential variations at points of steeply negative gradient (z ) or weakly positive gradient (z2), suggesting the proportionality (13.25a) between chemical diffusion rate and chemical potential gradient that characterizes the near-equilibrium state. Figure 13.2 Schematic depiction of chemical diffusion (arrows) induced by chemical potential variations at points of steeply negative gradient (z ) or weakly positive gradient (z2), suggesting the proportionality (13.25a) between chemical diffusion rate and chemical potential gradient that characterizes the near-equilibrium state.
Basically, using these technologies one would like to move forward to the theoretical optimum of a chemical process, which is that there are no other limitations than chemical kinetics. Normally a chemical process is influenced by more than just kinetics hydrodynamics (mixing), heat transfer, and mass transfer determine the quality of the process. Process intensification focuses on removing these three limitations to reaching the goal of kinetically limited processes. This is schematically depicted in Figure 2. [Pg.463]

In the above sections, nothing was said about the type of reaction between M and Q. This is because the Stem-Volmer equation is model independent, as explained above and also because eqs. (20)-(22) are for a diffusion-controlled reaction. Some information can be obtained regarding an electron transfer from various quenchers of similar chemical structures towards M. In this case, one may derive a relationship between ksv (as obtained from eq. (17)) and the ionization potential of these inhibitors. This is the Rehm-Weller equation, which is schematically depicted in fig. 4. In this plot, the plateau value corresponds to fcdin. For a general overview of problems related to electron transfers, see Pouliquen and Wintgens (1988) (in French). [Pg.488]

In SELEX, multiple rounds of in vitro transcription of random nucleic acid pools, affinity selection, and RT-PCR are performed, thus giving rise to exponential amplification of the selected molecules. The principle underlying SELEX is schematically depicted in Figure 1. After several selection cycles, the binders can subsequently be cloned and sequenced and then characterized. In SELEX, genotype and phenotype are simultaneously represented by the same RNA molecule, since it exerts its function through its three-dimensional structure, which is in turn determined by its nucleotide sequence. The chemical and functional diversity of RNA can be further increased by addition of cofactors such as histidine (Roth and Breaker, 1998) and divalent cations (Tarasow et al, 1997) to the selection. [Pg.375]

Figure 3.3.3 schematically depicts the basic structure of an electrochemical fuel cell device. Generally, in electrochemical cells the overall chemical redox reaction proceeds via two coupled, yet spatially separated half-cell redox reactions at two separate electrodes. [Pg.165]

The nature of the chemical moieties present is of course fundamental in determining the possible function of a molecule. Indeed, chemical behavior, such as reactivity, ability to produce ionic species, complexant power, reducing properties, etc., as well as physicochemical features, such as solubility and surface activity, are established by the presence of well-dehned groups, as schematically depicted in Table 37 a rigid division between chemical and physicochemical properties exclusively attributable to different chemical moieties can hardly be made, however. lonogenic groups, for instance, also provide hydrophilicity to the molecule in conjunction with the possibility of ion formation. [Pg.115]

FIGURE 13.23 Schematic depiction of possible ceria-silica removal mechanisms (a) primarily chemical, (b) surface chemical, and (c) enhanced mechanical. [Pg.387]

Fig. 15.19. Schematic depiction of the packing of strip-like and disk-like domains formed by the rod segments. (Reprinted with permission from Macromolecules, 1997, 30, 2110. 1997 American Chemical Society [67].)... Fig. 15.19. Schematic depiction of the packing of strip-like and disk-like domains formed by the rod segments. (Reprinted with permission from Macromolecules, 1997, 30, 2110. 1997 American Chemical Society [67].)...
Fig. 15.24. Schematic depiction of the polymerization of monomers within the vesicle bilayer leading to the formation of hollow nanospheres. (Reprinted with permission from Langmuir, 1998, 14, 1031. 1998 American Chemical Society [87].)... Fig. 15.24. Schematic depiction of the polymerization of monomers within the vesicle bilayer leading to the formation of hollow nanospheres. (Reprinted with permission from Langmuir, 1998, 14, 1031. 1998 American Chemical Society [87].)...
Shaker proteins in which various S4 residues were converted to cysteine were tested for their reactivity with a water-soluble cysteine-modifydng chemical agent that cannot cross the membrane. On the basis of whether the cysteines reacted with the agent added to one side or other of the membrane, the results indicated that in the resting state amino acids near the C-terminus of the S4 helix face the cytosol after the membrane is depolarized, some of these same amino acids become exposed to the exoplasmic surface of the channel. These experiments directly demonstrate movement of the S4 helix across the membrane, as schematically depicted in Figure 7-33 for voltage-gated Na" channels. [Pg.283]


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