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Bridged associational model

Because of the difficulties associated with Nagel s bridge-law model of reduction and the success of multiple realization arguments against type-identity materialism, Kim has come to reject type-identity materialism in favor of what he ealls functional reduction. The functional reduction of a property requires three steps ... [Pg.90]

The NBO procedure can be used to construct models allowing us to identify the major sources of destructive interference. In doing so, we focus on the l(n) compounds which have poly-norbomane bridges. Each model retains the localized n orbitals on the ethylenic groups as well as a subset of the NBOs associated with the bridge. HF/3-21G calculations are carried out on the l(n), n = 4, 6, 8, 10, and 12, molecules, and the canonical MOs are transformed to NBOs, which are used to construct a series of models shown in Figure 8. In terms of increasing sophistication these models are ... [Pg.831]

In Eq. (6) Ecav represents the energy necessary to create a cavity in the solvent continuum. Eel and Eydw depict the electrostatic and van-der-Waals interactions between solute and the solvent after the solute is brought into the cavity, respectively. The van-der-Waals interactions divide themselves into dispersion and repulsion interactions (Ed sp, Erep). Specific interactions between solute and solvent such as H-bridges and association can only be considered by additional assumptions because the solvent is characterized as a structureless and polarizable medium by macroscopic constants such as dielectric constant, surface tension and volume extension coefficient. The use of macroscopic physical constants in microscopic processes in progress is an approximation. Additional approximations are inherent to the continuum models since the choice of shape and size of the cavity is arbitrary. Entropic effects are considered neither in the continuum models nor in the supermolecule approximation. Despite these numerous approximations, continuum models were developed which produce suitabel estimations of solvation energies and effects (see Refs. 10-30 in 68)). [Pg.188]

Somoza EC, Winhusen TM, Bridge TP, et al An open-label pilot study of methylpheni-date in the treatment of cocaine-dependent patients with adult attention deficit/ hyperactivity disorder. J Addict Dis 23 77—92, 2004 Sora 1, Wichems C, Takahashi N, et al Cocaine reward models conditioned place preference can be established in dopamine- and in serotonin-transporter knockout mice. Proc Natl Acad Sci U S A 95 7699-7704, 1998 Soral, Hall FS, Andrews AM, etal Molecular mechanisms of cocaine reward combined dopamine and serotonin transporter knockouts eliminate cocaine place preference. Proc Nad Acad Sci U S A 98 5300-5305, 2001 Spear J, Alderton D Psychosis associated with prescribed dexamphetamine use 0etter). [Pg.208]

The formation of the PIC described above is based on the sequential addition of purified components in in vitro experiments. An essential feature of this model is that the assembly takes place on the DNA template. Accordingly, transcription activators, which have autonomous DNA binding and activation domains (see Chapter 39), are thought to function by stimulating either PIC formation or PIC function. The TAF coactivators are viewed as bridging factors that communicate between the upstream activators, the proteins associated with pol II, or the many other components of TFIID. This view, which assumes that there is stepwise assembly of the PIC—promoted by various interactions between activators, coactivators, and PIC components— is illustrated in panel A of Figure 37-10. This model was supported by observations that many of these proteins could indeed bind to one another in vitro. [Pg.351]

Figure 4.6 Left STM image of a stoichiometric 1 x 1 Ti02(l 1 0) surface, 14A x 14 A. Sample bias + 1.6 V, tunneling current 0.38 nA. The inset shows a ball-and-stick model of the unrelaxed 1 x 1 Ti02(l 1 0) surface. Rows of bridging oxygen atoms are labeled A and rows of fivefold coordinated titaniums B . Right contour plots of [0 1 l]-averaged charge densities associated with electron states within... Figure 4.6 Left STM image of a stoichiometric 1 x 1 Ti02(l 1 0) surface, 14A x 14 A. Sample bias + 1.6 V, tunneling current 0.38 nA. The inset shows a ball-and-stick model of the unrelaxed 1 x 1 Ti02(l 1 0) surface. Rows of bridging oxygen atoms are labeled A and rows of fivefold coordinated titaniums B . Right contour plots of [0 1 l]-averaged charge densities associated with electron states within...
The problems associated with the application of this (or any other) model have been discussed. Because of the form of the typical isotherm, which exhibits a broad plateau region, fitting of experimental results to the model requires that data be obtained over a very broad range of concentrations. This is often very difficult to accomplish in practice, especially when difference methods are used to determine the amount of polymer adsorbed. Evaluation of adsorption in real systems is further complicated by a lack of knowledge of the available solid surface area. The latter may be affected by particle size, shape and surface topography and by polymer bridging between particles. [Pg.35]

Knockout of the prolactin receptor, rather than knockout of prolactin, is necessary to explore the role of the hormone and its receptor in maternal behavior because several molecules other than prolactin, including growth hormone (GH) and placental lactogens, may stimulate the prolactin receptor. Disruption of the prolactin receptor gene in a mouse model has allowed for assessment of phenotypes associated with partial and complete prolactin receptor deficits (Goffin et ah, 1999). Prolactin receptor knockout mice have severe reproductive deficits. Heterozygous mothers (receptor —/+) were also unable to lactate (Bridges, 1998). [Pg.201]


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