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Local polarity

By covalently attaching reactive groups to a polyelectrolyte main chain the uncertainty as to the location of the associated reactive groups can be eliminated. The location at which the reactive groups experience the macromolecular environment critically controls the reaction rate. If a reactive group is covalently bonded to a macromolecular surface, its reactivity would be markedly influenced by interfacial effects at the boundary between the polymer skeleton and the water phase. Those effects may vary with such factors as local electrostatic potential, local polarity, local hydrophobicity, and local viscosity. The values of these local parameters should be different from those in the bulk phase. [Pg.53]

Moreover, despite the many advances in electrochemical measurement and modeling, our understanding of SOFC cathode mechanisms remains largely circumstantial today. Our understanding often relies on having limited explanations for an observed phenomenon (e.g., chemical capacitance as evidence for bulk transport) rather than direct independent measures of the mechanism (e.g., spectroscopic evidence of oxidation/reduction of the electrode material). At various points in this review we saw that high-vacuum techniques commonly employed in electrocatalysis can be used in some limited cases for SOFC materials and conditions (PEEM, for example). New in-situ analytical techniques are needed, particularly which can be applied at ambient pressures, that can probe what is happening in an electrode as a function of temperature, P02, polarization, local position, and time. [Pg.599]

It should be understood that even for micro surface features the potential is uniform and the ohmic resistance through the bath to peaks and valleys is about the same. Also, electrode potential against SCE will be uniform. What is different is that over micro patterns the boundary of the diffusion layer does not quite follow the pattern contour (Fig. 12.3). Rather, it thus lies farther from depth or vias than from bump peaks. The effective thickness, 8N, of the diffusion layer shows greater variations. This variation of 8N over a micro profile therefore produces a variation in the amount of concentration polarization locally. Since the potential is virtually uniform, differences in the local rate of metal deposition result if it is controlled by the diffusion rate of either the depositing ions or the inhibiting addition (leveling) agents. [Pg.214]

Conversely, Brooks and Johansson have calculated the spin-polarization term Ajp from a spin-polarized local-density approximation in atoms. These values can also be used in Eq. (3). The two evaluations, though not identical, do not differ greatly. [Pg.102]

The exciplexes with A values >0.2 eV and dipole moments which are smaller than those of the CT exciplexes are formed as a result of interactions between the CT state X(A D+) and non-polar (locally) excited complex states such as 1(A D) and 1(AD ) leading to stabilization of the CT state and to lowering of the dipole moment [116]. The coefficients Ci or C2, and C3 and C4 in the wave function (41) can be of comparable magnitude for such exciplexes. The value of A = 0.3 eV follows for the exciplex formed by the TPOB acceptor [l,3,5-tris(4-fert-butylphenyl-l,3,4-oxadiazolyl)benzene] with the TCTA donor [4,4/,4//-tri(A -carbazolyl) triphenyla-mine] based on EDOX = 0.69eV and EAred = —2.1eV, and the... [Pg.55]

Fig. 3. Solvent-solute localization and separation selectivity, (a) representation as in Fig. 2d of adsorption of mobile phase A/B (A, —nonpolar , —polar, nonlocalizing) (b) same for mobile phase A/C (C—polar, localizing) (c) adsorption of localizing solute X from mobile phase A/B (d) adsorption of nonlocalizing solute Y from mobile phase A/B (e) adsorption of X from mobile phase A/C (f) adsorption of Y from mobile phase A/C (g) completion of localized layer of molecules C at = 0.75 with maximum effect on solvent-solute localization selectivity. Fig. 3. Solvent-solute localization and separation selectivity, (a) representation as in Fig. 2d of adsorption of mobile phase A/B (A, —nonpolar , —polar, nonlocalizing) (b) same for mobile phase A/C (C—polar, localizing) (c) adsorption of localizing solute X from mobile phase A/B (d) adsorption of nonlocalizing solute Y from mobile phase A/B (e) adsorption of X from mobile phase A/C (f) adsorption of Y from mobile phase A/C (g) completion of localized layer of molecules C at = 0.75 with maximum effect on solvent-solute localization selectivity.
Fig. 8. Dependence of C-solvent strength ( on coverage of adsorbent surface 0. Mixtures A/C of nonpolar solvent A and polar localizing solvent C , isopropanol/hexane/silica , acetone/hexane/silica , ethyl ether/hexane/silica/ V, ethyl ether/pentane/silica O, isopropyl ether/pentane/alumina. Data taken from Snyder and Glujch (14) and Hara et al. (25). Curves through data are best fit to Eqs. (12) and (40). Fig. 8. Dependence of C-solvent strength ( on coverage of adsorbent surface 0. Mixtures A/C of nonpolar solvent A and polar localizing solvent C , isopropanol/hexane/silica , acetone/hexane/silica , ethyl ether/hexane/silica/ V, ethyl ether/pentane/silica O, isopropyl ether/pentane/alumina. Data taken from Snyder and Glujch (14) and Hara et al. (25). Curves through data are best fit to Eqs. (12) and (40).
Alternatively, dipolar-coupling frequencies can be determined by observing the transfer of polarization between coupled spins. Clearly, an initial density operator that describes polarization localized on a given spin, say k, (cr(0) oc Skz) does not commute with the Hamiltonian of Equations (4.1) and... [Pg.86]

Peters, V., Becher, D., and Rehm, B.H.A. (2007) The inherent property of polyhydroxyalkanoate synthase to form spherical PHA granules at the cell poles the core region is required for polar localization. J. Biotechnol., 132, 238-245. [Pg.270]

We examined the effect of coupling between surface plasmon polariton (SPP) modes on the optical activity of metal nanostructures. By measuring the in-plane wave vector dependence on transmission and polarization azimuth rotation, we show that coupling of the SPP modes with orthogonal polarization localized at different interfaces is responsible for the optical activity in metal nanostructures. [Pg.81]

Fig. 2 Experimental setup for scanning pyroelectric microscopy (SPEM). As indicated, the sample may consist of two domains of opposite polarization. Local heating in either domain of polarization produces excess charges at both ends of the polar axis. This induces a current flow in the outer circuit. Opposite polarity is seen because of a change in the current direction. Fig. 2 Experimental setup for scanning pyroelectric microscopy (SPEM). As indicated, the sample may consist of two domains of opposite polarization. Local heating in either domain of polarization produces excess charges at both ends of the polar axis. This induces a current flow in the outer circuit. Opposite polarity is seen because of a change in the current direction.
Schindelman G., Morikami A., Jung J., Baskin T.I., Carpita N.C., Derbyshire R, McCann M.C., and Benfey P.N. 2001. COBRA encodes a putative GPI-anchored protein, which is polarly localized and necessary for oriented cell expansion in Arabidopsis. Genes and Development 15 1115-1127. [Pg.198]

Bianchi, J. Rose, R. C. 1985. Transport of L-ascorbic acid and dehydro-L-ascorbic acid across renal cortical basolateral membrane vesicles. Biochim. Biophys. Acta 820(2) 265-273. Bode, A. M. Yavarow, C. R. 1993. Enzymatic basis for altered ascorbic acid and dehydro-ascorbic acid levels in diabetes. Biochem. Biophys. Res. Commun. 191 1347-1353. Biondi, C. Pavan, B. Dalpiaz, A. Medici, S. Lunghi, L. Vesce, F. 2007. Expression and characterization of vitamin C transporter in the human trophoblast cell line HTR-8/ SVneo Effect of steroids, flavonoids, and NSAIDs. Mol. Hum. Reprod 13(1) 77-83. Boyer, J. C. Campbell, C. E. Sigurdson, W. J. Kuo, S. M. 2005. Polarized localization of vitamin C transporters, SVCTl and SVCT2, in epithelial cells. Biochem. Biophys. Res. Commun. 334 150-156. [Pg.271]

Steinmann, T., Geldner, N., Grebe, M. et al. (1999). Coordinated polar localization of auxin efflux carrier PINl by GNOM ARF GEE Science, 286,316-318. [Pg.202]

Merocyanines are widely used as solvatochromic dyes. Fujita et al. demonstrated that the Brooker s dye analogue (Fig. 32, 24) shows a colour change based on protonation and deprotonation in a densely packed SAM (Fig. 32, 24) [196]. Surface plasmon spectroscopy and X-ray photoelectron spectroscopy indicate that the monolayers are closely packed. The layer thickness is consistent with the molecules having a tUt angle of 30° to the surface normal IRRAS spectroscopy shows that the chromophores are located in a polar local dielectric situation even in non-polar solvents. Nonetheless, the deprotonated, zwitterionic form of the dye shows a distinct negative solva-tochromism depending on the solvent polarity. [Pg.285]


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See also in sourсe #XX -- [ Pg.71 , Pg.72 ]

See also in sourсe #XX -- [ Pg.13 ]




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Localized polarity

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