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McConnell

Theoretical models of the film viscosity lead to values about 10 times smaller than those often observed [113, 114]. It may be that the experimental phenomenology is not that supposed in derivations such as those of Eqs. rV-20 and IV-22. Alternatively, it may be that virtually all of the measured surface viscosity is developed in the substrate through its interactions with the film (note Fig. IV-3). Recent hydrodynamic calculations of shape transitions in lipid domains by Stone and McConnell indicate that the transition rate depends only on the subphase viscosity [115]. Brownian motion of lipid monolayer domains also follow a fluid mechanical model wherein the mobility is independent of film viscosity but depends on the viscosity of the subphase [116]. This contrasts with the supposition that there is little coupling between the monolayer and the subphase [117] complete explanation of the film viscosity remains unresolved. [Pg.120]

McConnell et al. [196] and Andelman and co-workers have predicted [197,198] an ordered array of liquid domains in the gas-liquid coexistence regime caused by the dipole moment difference between the phases. These superstructures were observed in monolayers of dipalmitoyl phosphatidylcholine monolayers [170]. [Pg.132]

The free energy of a monolayer domain in the coexistence region of a phase transition can be described as a balance between the dipolar electrostatic energy and the line tension between the two phases. Following the development of McConnell [168], a monolayer having n circular noninteracting domains of radius R has a free energy... [Pg.136]

In principle, compressing a monolayer should produce more domains of radius J eq. however McConnell shows that in practice, domains grow to exceed this radius. Once a domain grows to A = it becomes unstable toward... [Pg.139]

The effects of electric fields on monolayer domains graphically illustrates the repulsion between neighboring domains [236,237]. A model by Stone and McConnell for the hydrodynamic coupling between the monolayer and the subphase produces predictions of the rate of shape transitions [115,238]. [Pg.139]

Fig. XV-8. Fluorescence micrographs of crystalline domains of an S-DPPC monolayer containing 2% cholesterol and compressed to the plateau region. [From H. McConnell, D. Keller, and H. Gaub, J. Phys. Chetn., 40, 1717 (I486) (Ref, 49). Copyright 1986, American Chemical Society.]... Fig. XV-8. Fluorescence micrographs of crystalline domains of an S-DPPC monolayer containing 2% cholesterol and compressed to the plateau region. [From H. McConnell, D. Keller, and H. Gaub, J. Phys. Chetn., 40, 1717 (I486) (Ref, 49). Copyright 1986, American Chemical Society.]...
McConnell H M 1958 Reaction rates by nuclear magnetic resonance J. Chem. Phys. 28 430-1... [Pg.2112]

The simplest theoretical orbital-based estimate of the coupling interaction, is provided by the McConnell relation ... [Pg.2979]

Coupling constants, calculated with the aid of McConnel s formula (286) are given in Table 1-42 together with the experimental values. [Pg.85]


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Bloch-McConnell equations

Electron McConnell equation

McConnel equation

McConnell crystals

McConnell equation

McConnell equation double bond

McConnell expression

McConnell model

McConnell relation

McConnell relationship

McConnell solids

McConnell superexchange mechanism

McConnell, Harden

McConnell, James

McConnell-Hoffman-Metzger

McConnell-Robertson equation

McConnells Model

McConnell’s equations

McConnell’s model

McConnell’s relation

Organic McConnell proposal

Superexchange McConnell model

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