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McConnell’s model

Use the reasoning of McConnell s model (Eq.4.27) to predict the ground state of the benzyl dimer with the CH2 groups in ortho and for the conformer where the two units are perfectly aligned. [Pg.112]

McCONNELL S HEITLER-LONIXJN SPIN-EXCHANGE MODEL BETWEEN SPIN DENSITIES OF OPPOSITE SIGN ON RADICALS A AND B... [Pg.227]

Fig. 21 Schematic representation of strategies for spin alignment in D/A salts or complexes by application of spin conservation in different electron configurations of interacting molecular orbitals, (a) Typical D/A interaction between two closed-shell D and A, (b and b ) McConnell s proposal, (c) Breslow s extension, (d) Torrance s model, (e) Wudl s model, and (f) Chiang s model for further doping. Fig. 21 Schematic representation of strategies for spin alignment in D/A salts or complexes by application of spin conservation in different electron configurations of interacting molecular orbitals, (a) Typical D/A interaction between two closed-shell D and A, (b and b ) McConnell s proposal, (c) Breslow s extension, (d) Torrance s model, (e) Wudl s model, and (f) Chiang s model for further doping.
McConnell s Heitler-London spin-exchange model between spin densities of opposite sign on radicals A and B 227 Ferromagnetic coupling in donor-acceptor salts 230 Model experiments and realization of ferromagnetic interactions 232... [Pg.179]

McConnell s heitler-london spin-exchange model between... [Pg.227]

Fig. 6. Schematic model of two-phase system, with solid domain S in equilibrium with fluid domain F. The relative proportions, and compositions of F and S are determined from, for example, the phase diagram in Fig. 2. The 13C nuclear resonance spectra of lipids in the solid phase S are broader than the nuclear resonance spectra of lipids in the fluid phase F the spectra of lipids in the fluid phase F can be broadened if they diffuse to, and stick to, the solid phase. For a detailed theoretical calculation of line widths expected for this geometry, see Ref. 4. The bilayer length is L, and the domain boundary is b - b. [Reprinted with permission from P. Brulet and H. M. McConnell, J. Am. Chem. Soc., 98, 1314 (1977). Copyright by American Chemical Society.]... Fig. 6. Schematic model of two-phase system, with solid domain S in equilibrium with fluid domain F. The relative proportions, and compositions of F and S are determined from, for example, the phase diagram in Fig. 2. The 13C nuclear resonance spectra of lipids in the solid phase S are broader than the nuclear resonance spectra of lipids in the fluid phase F the spectra of lipids in the fluid phase F can be broadened if they diffuse to, and stick to, the solid phase. For a detailed theoretical calculation of line widths expected for this geometry, see Ref. 4. The bilayer length is L, and the domain boundary is b - b. [Reprinted with permission from P. Brulet and H. M. McConnell, J. Am. Chem. Soc., 98, 1314 (1977). Copyright by American Chemical Society.]...
Fomichev, V.I., W.E. Ward, S.R. Beagley, C. McLandress, J.C. McConnell, N.A. McFarlane, and T.G. Shepherd, Extended Canadian Middle Atmosphere Model Zonal-mean climatology and physical parameterizations. J Geophys Res 107, DIO, doi 10.1029/2001JD000479, 2002. [Pg.253]

A number of different techniques have been applied to test the distance and orientation dependence of ET reactions (Closs and Miller, 1988 Closs et al, 1989 Liang et al, 1990 Reimers and Hush, 1990 Fox and Chanon, 1988 Wasielewski, 1989 Paddon Row and Jordan, 1988 Joachim et al, 1990 McConnell, 1961). Our method of analysing the mode of charge distribution in charged species is esr spectroscopy, which defines the timescale of the detectable dynamic species (Gerson, 1967 Kurreck et al, 1988 Wertz and Bolton, 1972). If an electron transfer is slow relative to the esr timescale (< 10 7 s) the spectrum corresponds to that of monomeric model compounds with a single electrophore. If the hopping process is rapid on the esr timescale, one will detect an effective delocalization. [Pg.21]

K) [68]. Decamethylmanganocenium is a d high-spin (S = 1) system, as opposed to the d low-spin (S = 1/2) ferrocenium cation. Bulk ferromagnetism has also been reported for the decamethylchromocene/TCNQ [69] CT complex and for [MnCpf] [TCNQ] " [70]. These two latter materials have shown that the interpretation of their ferromagnetism cannot be based on the simple McConnell model, which invokes a configurational mixing of a virtual CT state (vide supra). [Pg.464]

Wurster s Blue perchlorate has been the subject of many investigations. Its stability as a solid and in solution, its ease of preparation, and its symmetry make it an ideal model in spectroscopic and magnetic susceptibility studies. It was one of the first cation radicals to be shown to exist both as a monomer and as a dimer in solution (Hausscr, 1956 Bolton et al., 1962) and in the solid state (Duffey, 1962 McConnell and Lynden-Bell, 1962), the dimeric form being obtainable reversibly by lowering the temperature. This phenomenon is widespread among cation radicals and is discussed in section 3. [Pg.193]

At Stanford, Harden M. McConnell developed a new technique, called spin labelling, based upon EPR spectroscopy. While carbon-centered free radicals are extremely reactive and short-lived, radical oxides of nitrogen, such as NO and NO2, are moderately stable. McConnell noted that nitroxyl radicals (RR N-O) are extremely stable if R and R are tertiary and can be chemically attached to biological molecules of interest. In 1965, he published the concept of spin labeling and, in 1966, demonstrated that a spin-labelled substrate added to a-chymotrypsin forms a covalent enzyme-substrate complex. The EPR signal was quite broad suggesting restricted motion consistent with Koshland s induced-fit model. In 1971, McConnell published a smdy in which spin labelling indicated flip-flop motions of lipids in cell membranes. This was the start of dynamic smdies of cell membranes. [Pg.247]


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See also in sourсe #XX -- [ Pg.110 ]




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