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High mobility cations

Similarly short lifetimes are expected for branched alkanes, such as isooctane [22]. Due to these lifetime limitations, the chemical behavior of cycloalkane holes is understood in more detail than that of the solvent holes in other hydrocarbon liquids. [Pg.178]

From conductivity studies, it is known that the cycloalkane holes rapidly react with various solutes, typically by electron or proton transfer [7-19]. These scavenging reactions establish the identity of the high-mobility cations as the solvent holes Rapid generation of aromatic radical cations (A +) in reactions of the holes with aromatic solutes (A) was observed using pulse radiolysis - transient absorption spectroscopy [4,5,6,20,23-25] and, more recently, using pulse-probe laser-induced dc conductivity [26]. Rapid decay of the conductivity and transient absorbance signals from the cycloalkane holes was also observed [4-25]. [Pg.178]

It has long been speculated that the high-mobility solvent holes exist in hydrocarbons other than the four cycloalkanes. Recently, high-mobility solvent holes were observed in 2,6,10,15,19,23-hexamethyltetracosane (squalane) [24] and in cyclooctane [27]. In the squalane, rapid electron-transfer reactions of solvent holes with low-IP solutes were observed using transient absorbance spectroscopy and magnetic resonance [24]. Fast diffusion and high-rate [Pg.178]


Fig. 5 Effect of molecular size on the relative importance of electrorepulsion (ER) and electroosmosis (EO) to the overall iontophoretic transport of cations and anions. Small, highly mobile cations are principally moved across the skin by ER. But, as molecular size increases, the fraction of charge carried by a cationic drug decreases, and the principal mechanism of transport becomes EO. For anions, on the other hand, EO is a negative contribution to the total flux and, once the molecular size reaches a critical value (me, completely cancels out the ER contribution to electrotransport (resulting in no net flux). Fig. 5 Effect of molecular size on the relative importance of electrorepulsion (ER) and electroosmosis (EO) to the overall iontophoretic transport of cations and anions. Small, highly mobile cations are principally moved across the skin by ER. But, as molecular size increases, the fraction of charge carried by a cationic drug decreases, and the principal mechanism of transport becomes EO. For anions, on the other hand, EO is a negative contribution to the total flux and, once the molecular size reaches a critical value (me, completely cancels out the ER contribution to electrotransport (resulting in no net flux).
Sauer, M. C. and Schmidt, K. H., The decay of the high-mobility cation in cyclohexane, Radiat. Phys. Chem., 32, 281,1988. [Pg.151]

Particular interest in the study of copper and silver chalcogenides is determined by the fact that in these systems cations exhibit abnormally high mobility. A number of studies attempt to explain the emeigence of highly mobile cations by the stmctural features of the band, and the hybridization degree of the d-levels of the metal and p-levels of chalcogen in... [Pg.168]

A different type of switch is displayed in Fig. 2.40. Here, a Ru-bipy complex is appended to a calixarene in which two of the phenoxyl groups have been oxidized to quinones, complex 90 [233, 234]. The calixarene also possesses a pendant bipyridine ligand. Upon illumination into the MLCT band localized on the metal complex, light-induced electron transfer takes place from the triplet state of Ru-bipy to one of the quinones. This process involves diffusive encounter between the reactants and it should be noted that NMR and molecular dynamics simulations indicate that the calixarene walls are highly mobile. Cations, such as Ba +, bind to the lower rim of the calixarene and are held in place by the additional bipyridine ligand. This has the effect of forcing the pendant Ru-bipy away from the calixarene in order to minimize electrostatic repulsion. The net effect is to curtail light-induced electron transfer. Thus, whereas 90 is nonluminescent the various cation-... [Pg.73]

As described in Section 10-, the bonding in solid metals comes from electrons in highly delocalized valence orbitals. There are so many such orbitals that they form energy bands, giving the valence electrons high mobility. Consequently, each metal atom can be viewed as a cation embedded in a sea of mobile valence electrons. The properties of metals can be explained on the basis of this picture. Section 10- describes the most obvious of these properties, electrical conductivity. [Pg.780]

The effect of highly polarizable cations on transport properties has scarcely been studied. Since the nitrate melts of Ag and TL are stable and have high polarizabilities, as shown in Table 5, their internal mobilities in binary mixtures containing one or both of these cations have been measured frequently. The isotherms are shown for and m,., in Figs. 10 and 11,... [Pg.138]

The Effeet of Highly Polarizable Cations on the Internal Mobility of the Seeond Cation in (Mi, M2)N03... [Pg.143]

When water undergoes self-ionization, a range of cationic species are formed, the simplest of which is the hydronium ion, HjO (Clever, 1963). This ion has been detected experimentally by a range of techniques including mass spectrometry (Cunningham, Payzant Kebarle, 1972), as have ions of the type H+ (HaO) with values of n up to 8. Monte-Carlo calculations show that HjO ions exist in hydrated clusters surrounded by three or four water molecules in the hydration shell (Kochanski, 1985). These ions have only a short lifetime, since the proton is highly mobile and may be readily transferred from one water molecule to another. The time taken for such a transfer is typically of the order of 10 s provided that the receiving molecule of water is correctly oriented. [Pg.44]

The impedance of the system described above will generally consist of in parallel with Cg, i.e. only the bulk electrolyte between the metal electrode and the reference electrode is likely to make a contribution to the impedance. Although Qi in parallel with R t is theoretically present at sufficiently low frequencies it is only measurable in special circumstances - for example when the metal cations have an unusually high mobility so that Rq is comparatively small, enabling R i to be observed. [Pg.283]


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See also in sourсe #XX -- [ Pg.178 ]




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