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Polarization tion transfer

Effects of solvent polarity, counter-anion nucleophilidty, temperature, and monomer concentration on the carbenium ion polymerization chemistry have been extensively studied29,36 38,49. Based on previous knowledge26"29 Me3Al was chosen because with this coinitiator undesired chain transfer to monomer processes are absent. Preliminary experiments showed that Et3Al coinitiator did not yield PaMeSt, possibly because the nuc-leophilicity of the counter-anion Et3AlQe is too high and thus termination by hydrida-tion is faster than propagation36. ... [Pg.31]

Fig. 8-8. Energy levels for redox electron transfer reaction at a metal electrode (a) in equilibrium, (b) in anodic polarization with reao tion rate determined by interfadal electron transfer, (c) anodic polarization with reaction rate determined by both interfadal electron transfer and diffusion of hydrated partides. EF0)Eooxj.a= Fenni level of redox electrons at an interface. Fig. 8-8. Energy levels for redox electron transfer reaction at a metal electrode (a) in equilibrium, (b) in anodic polarization with reao tion rate determined by interfadal electron transfer, (c) anodic polarization with reaction rate determined by both interfadal electron transfer and diffusion of hydrated partides. EF0)Eooxj.a= Fenni level of redox electrons at an interface.
In this study, benzaldehyde and benzaldehyde-methyllithium adduct were fully optimized at HF/6-31G and their vibrational frequencies were calculated. The authors used MeLi instead of lithium pinacolone enolate, since it was assumed that the equilibrium IBs are not much different for the MeLi addition and lithium enolate addition. Dehalogena-tion and enone-isomerization probe experiments detected no evidence of a single electron transfer to occur during the course of the reaction. The primary carbonyl carbon kinetic isotope effects and chemical probe experiments led them to conclude that the reaction of lithium pinacolone enolate with benzaldehyde proceeds via a polar mechanism. [Pg.36]

Consider then the scenario in Fig. 18, and suppose that we wish to tram population from L to >. Then, since Et d e Ej) differ for the L and D stal we can choose a laser polarization such that this matrix element is zero for exci tion of the ground state of D but not L. Application of a ttpulse at this poladzal will then transfer the ground state L population to the excited state. Applicatij of a second tt pulse of different polarization can then transfer this population the excited vibrational state of the ground electronic state of D, by now choosi a polarization that does not couple the excited state to L. [Pg.86]

The described problem was encountered in investigations of cis-trans isomeriza-tions and cycloadditions of donor olefins D and acceptor olefins A in acetonitrile. All polarizations, both of the cycloadducts and of the starting and isomerized olefins, could be traced to radical ion pairs D" + A" formed by photoinduced electron transfer. As, however, exciplexes are frequently discussed as percursors to the products in such systems,and CIDNP does not respond to exciplexes because no diffusive separation is possible, the question as to the relative contributions of the radical ion and exciplex pathways arose. To answer it, we employed photoinduced electron transfer sensitization (PET-sensitization). [Pg.193]

Other counter-ions may be exchanged with the bulk non-polar phase, provided something is able to solubilize them there. This will usually be in the form of an ion-pair with a species better solvated by the medium. For example, an acid with a large hydrophobic group may form a Na+ salt with sufficient solubility in the bulk medium. The protonated acid will carry H+ to and from the enzyme in exchange, to maintain electroneutrality. A similar process with a hydrophobic amine, for example, can transfer H+ and Cl-. Solubilization of the small ion may be aided by complexa-tion, for example of Na+ by a crown ether. The exchanges can be written as ... [Pg.283]


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See also in sourсe #XX -- [ Pg.230 ]




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