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Migration/trapping systems

In subsection (B) we will discuss the results with the anthracene energy trap more extensively, from the point of view of intrachain energy migration. This system is more difficult to analyze with simple models because of the large Forster radius for naphthalene to anthracene single-step energy transfer (25A ) ... [Pg.405]

Nearly all reservoirs are water bearing prior to hydrocarbon charge. As hydrocarbons migrate into a trap they displace the water from the reservoir, but not completely. Water remains trapped in small pore throats and pore spaces. In 1942 Arch/ e developed an equation describing the relationship between the electrical conductivity of reservoir rock and the properties of its pore system and pore fluids. [Pg.147]

We have also examined the behavior of copolymers of o-tolyl vinyl ketone and methyl vinyl ketone (CoMT). In this case the light is absorbed exclusively at the aromatic carbonyl chromophore and the reaction proceeds from this site, while the methyl vinyl ketone moieties provide a relatively constant environment but prevent energy migration along the chain. The values of Tg and Tip in benzene have been included in Table II. These copolymers axe also soluble in some polar solvents for example, we have used a mixture of acetonitrile acetone methanol (30 30 Uo, referred to as AAM). This mixture is also a good solvent for the electron acceptor paraquat (PQ++) which has been shown to be good biradical trap in a number of other systems (9.). [Pg.23]

If there is no interaction between similar reactants (traps) B, they are distributed according to the Poisson relation, Ab (r, t) = 1. Besides, since the reaction kinetics is linear in donor concentrations, the only quantity of interest is the survival probability of a single particle A migrating through traps B and therefore the correlation function XA(r,t) does not affect the kinetics under study. Hence the description of the fluctuation spectrum of a system through the joint densities A (r, ), which was so important for understanding the A4-B — 0 reaction kinetics, appears now to be incomplete. The fluctuation effects we are interested in are weaker here, thus affecting the critical exponent but not the exponential kinetics itself. It will be shown below that adequate treatment of these weak fluctuation effects requires a careful analysis of many-particle correlations. [Pg.271]

These bacteria cannot in general oxidize water and must live on more readily oxidizable substrates such as hydrogen sulfide. The reaction centre for photosynthesis is a vesicle of some 600 A diameter, called the chromato-phore . This vesicle contains a protein of molecular weight around 70 kDa, four molecules of bacteriochlorophyll and two molecules of bacteriopheophy-tin (replacing the central Mg2+ atom by two H+ atoms), an atom Fe2+ in the form of ferrocytochrome, plus two quinones as electron acceptors, one of which may also be associated with an Fe2+. Two of the bacteriochlorophylls form a dimer which acts as the energy trap (this is similar to excimer formation). A molecule of bacteriopheophytin acts as the primary electron acceptor, then the electron is handed over in turn to the two quinones while the positive hole migrates to the ferrocytochrome, as shown in Figure 5.7. The detailed description of this simple photosynthetic system by means of X-ray diffraction has been a landmark in this field in recent years. [Pg.169]

A potential difference across the NB/water interface (Ao 0) is determined by the concentrations of TBA+ dissolved in both phases, and calculated to be —131 mV on the basis of Eq. 4. A standard ion transfer potential of ferrocene has been reported to be -75 mV [96]. Therefore, FeCp-EtOH+ is likely to exit quickly to the water phase across the droplet/water interface at the present Ao . Diffusion of FeCp-EtOH + in the NB and water phases is thus concluded to be the rate-determining step of MT from GE to CE across the droplet/water interface. If the Ao value is higher than the ion transfer potential of FeCp-EtOH+ in the NB/water system, a slow MT process, such as migration of the compound across the interface, will be detected. A combination of laser trapping with the microelectrode array methods is highly useful for studying directly MT processes between a droplet and the surrounding solution phase. [Pg.197]


See other pages where Migration/trapping systems is mentioned: [Pg.4]    [Pg.4]    [Pg.233]    [Pg.256]    [Pg.353]    [Pg.475]    [Pg.93]    [Pg.2500]    [Pg.82]    [Pg.449]    [Pg.19]    [Pg.465]    [Pg.237]    [Pg.271]    [Pg.606]    [Pg.78]    [Pg.478]    [Pg.1053]    [Pg.172]    [Pg.146]    [Pg.177]    [Pg.188]    [Pg.210]    [Pg.14]    [Pg.14]    [Pg.140]    [Pg.85]    [Pg.813]    [Pg.402]    [Pg.3]    [Pg.3]    [Pg.107]    [Pg.40]    [Pg.216]    [Pg.15]    [Pg.107]    [Pg.19]    [Pg.254]    [Pg.256]    [Pg.274]    [Pg.214]    [Pg.111]    [Pg.196]    [Pg.1008]   
See also in sourсe #XX -- [ Pg.4 ]




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Trapping systems

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