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Isolated model

Tab. 3.3 Main structural data defining the optimized heme-CO complex for each protein conformation l-V. The last row corresponds to the results obtained for the heme-CO isolated model (Section 3.3.1). [Pg.102]

Both a-silane and a-dihydrogen complexes are useful and in some cases isolable models for the rarely observed a-alkane complexes. Unfortunately, silane complexes of Pt(II) are generally dinuclear (37,122) rendering them less desirable models for Pt(II) a-alkane complexes. In contrast, the closely related dihydrogen complexes of Pt(II) are mostly monomeric (123-126). [Pg.282]

The procedures used for these two polymers were different because a full description of DeS had been published by Mitra et al. (16) but no three-dimensional structure was available for Hep. In both cases, helical symmetry was iirposed so that each residue "sees" the same environment. The final DeS model included sodium ions and water as well as adjacent chains while only an isolated model of Hep was constructed. [Pg.335]

Figure 5. Series of IR femtosecond/picosecond laser pulses for the sequence of transitions OH(u = 10)- OH(u = 15) - 0 + H for the isolated model OH cf. Fig. 1 and Table I. The notations are as in Fig. 3 populations Pwen(t) = Xoio Po( ) and PCOnt(t) = lPweiKO indicate the total populations of bound and continuum states embedded in the potential well and above the dissociation threshold, respectively. The resulting spectrum of ATD is shown in Fig. 1. Figure 5. Series of IR femtosecond/picosecond laser pulses for the sequence of transitions OH(u = 10)- OH(u = 15) - 0 + H for the isolated model OH cf. Fig. 1 and Table I. The notations are as in Fig. 3 populations Pwen(t) = Xoio Po( ) and PCOnt(t) = lPweiKO indicate the total populations of bound and continuum states embedded in the potential well and above the dissociation threshold, respectively. The resulting spectrum of ATD is shown in Fig. 1.
The evidence for the proposed mechanism as shown in Fig. 7.8 comes mainly from in situ NMR studies and X-ray structures of isolated model complexes. Rapid equilibrium between species 7.25 to 7.27 involving an 7j3-allyl type of interaction results in a species of the type 7.28. This species has been observed by NMR. Similar model complexes such as 7.29 and 7.30 have been characterized by single crystal X-ray studies. [Pg.146]

The degree of ligand dissociation is dependent on donor and 77-acceptor strength, i.e., neither strongly basic trialkylphosphines nor ligands such as CO dissociate as readily as triarylphosphines in most circumstances. For this reason complexes of trialkylphosphines often provide isolable models for catalytically active species... [Pg.1168]

This contribution deals with the use of ultraviolet photoelectron spectroscopy (UPS) for the study of the surface and bulk electronic structure of organic molecular and polymeric solids. In so far as is necessary, some features of the UPS of isolated model monomer molecules in the gas phase are described in order to provide a basis for an understanding of certain phenomena that occur in the corresponding condensed molecular and polymeric solids. Some features of photoelectron spectroscopy in general are outlined with an emphasis on the phenomenological interpretation of spectra for the several case studies to be reviewed. The complimentary nature of X-ray photoelectron spectroscopy (XPS or sometimes ESCA) and UPS is pointed out. The discussions presented are focused upon the experimental aspects of the UPS of insulating organic molecular and polymeric solids, but specific hardware considerations are not included. A variety of references, some of a review nature, are included, but the content is not intended to be historically complete. Examples for examination are drawn primarily from the author s own experience. [Pg.121]

Fig. 3. Experimental adsorption Isotherm ofN2 on SWNH at 77 K (o) and simulated isotherms of Nj on three models at 77 K triangular array (+ symbols) square array ( ) adsorption on the external surface of an isolated model (A). [Pg.40]

The Intention of this volume is to give a flavour of the types of problems in biochemistry that theoretical calculations can solve at present, and to illustrate the tremendous predictive power these approaches possess. With these aspects in mind, I have tried to gather some of the leading scientists in the field of theoretical/computational biochemistry and let them present their work. You will hence find a wide range of computational approaches, from classical MD and Monte Carlo methods, via semi-empirical and DFT approaches on isolated model systems, to Car-Parrinello QM-MD and novel hybrid QM/MM studies. The systems investigated also cover a broad range from membrane-bound proteins to various types of enzymatic reactions as well as inhibitor studies, cofactor properties, solvent effects, transcription and radiation damage to DNA. [Pg.710]

By contrast, the in situ cannulation of veins that drain specific areas of the gut and the collection of all the effluent blood from this area (which is replaced by continuous infusion of blood into the cannula) has all the advantages of the totally isolated model. The major difficulty with this model is the ability to control the blood pressure and flow from the dosed area of the gut. [Pg.463]

A comparison of the results of Biro and Szent-Gyorgyi (1949) with those of Korey (1950) reveals a similar parallehsm between breakdown and structural changes in the protein. In these experiments, it is true, the measured hydrolysis rate does not represent an initial velocity, but the second of the conditions under (ii) above is fulfilled, for the preparations were as free to contract in the contraction experiments as in the enzymatic. The optimum ATP concentration found for shortening (Korey, 1950) and for breakdown (Biro and Szent-Gyorgyi, 1949) are both 10 for extracted fiber bundles at 20°C. The fact that this value is higher than for the isolated model fiber may be only an apparent discrepancy, for the effective concentration of ATP in the interior of the fiber bundle is appreciably lower than that in the bath. [Pg.186]

The first problem originates from the structural complexity of zeohte frameworks which normally contain several hundred atoms per unit cell. This makes studies of the vibrational behavior of the lattice and the search for modes characteristic of special structural units even more difficult. In this case, a usual approximation is to cut out an isolated model cluster from the framework and treat it hke a molecule. In comparison with quantum mechanics, in NCA it is not necessary to saturate the dangfing bonds of the cluster by terminal pseudoatoms (vide infra). In a first attempt, based on such an assumed decoupHng of modes from the surrounding framework, Blackwell [7] predicted vibrational frequencies... [Pg.15]

Note that using an isolated system automatically ensures that we will compare states having the same values of two state variables, U and V, our two constraints. We insert the postulate that entropy increases with U to ensure that the other directionality parameters to be derived decrease (have minima) rather than increase. This can be shown by considering the isolated (model) system in Figure 4.1. [Pg.70]

Careful mechanistic studies on the carbonylation process have been reported by Yamamoto, including studies with isolated model compounds. - These studies have revealed several reaction pathways, and the particular pathway depends on whether the electrophile is an aryl or benzyl halide and whether the nucleophile is an amine or an alkoxide. The existing experimental data suggest that the latter pathway b in Scheme 17.29 involving insertion of CO into the palladium-aryl bond to form a benzoylpalladium halide intermediate occurs. These complexes have been isolated with PMe and PPhj as ligand and have been shown to form the ester product upon reaction with an alcohol and amine base and to form the amide products upon reaction with amine alone. [Pg.797]

A complete theory of the hierarchical mechanism of dynamic synaptic activity would require the study of co-operation and competition among the three oscillators. Here only one model, established for explaining the slow oscillation will be presented. The isolated model shows periodic behaviour. [Pg.189]

Non-linear finite-element models of high damping rubber bearings have been developed and implemented in the ABAQUS code in the framework of Italian cooperative studies for seismic isolation development. The Hyperelastic models used have been based on the results of tests on rubber specimens. The isolators models are validated through comparison of numerical results with complete bearing test data. [Pg.139]

The availability of reliable isolators models will allow the number of quite costly experimental tests on complete bearings to be considerably limited, not only as regards the analysis of the effects of some important parameters (e.g. temperature, ageing, vertical load on horizontal stiffness, etc.), but also for complicated experiments such as for instance, failure tests and analysis of the effects of defects. [Pg.139]

Using the isolable model alkylcobalt tetracarbonyl, CH3CH2 0(C=0)CH2Co(CO)4, the kinetics of both types of reductions has been determined (164). The rate of ethyl acetate formation is first order in CH3CH2 0(C=0)CH2Co(CO)4 and close to negative first order in carbon monoxide. [Pg.1099]

If hybridization of orbitals has turned out to be a sterile device in the context of the preceding section, it was because the quadrupolar field cannot distinguish between sp hybrids that are oppositely directed. Needless to say, hybridization is much too important a concept in chemical bonding to be abandoned. What makes it important, however, is the enhanced electrostatic attraction of an electron in a suitably directed hybrid orbital of one atom towards the nucleus of another. This effect can be simulated by putting our isolated model atom in a dipolar field lined up along the x axis, in which the potential increases with X. An electron in that atom will be stabilized in regions of positive potential x > 0) and destabilized where x - and the potential - are negative. We do this in two ways ... [Pg.42]

The Madelung potentials, corrected for edge effects, were added to the Fock operator of the prototype molecule. The geometrical parameters were kept at the values optimized for the isolated model, involving the interaction with the NH3 molecule, in both the neutral and ionic forms, at the 6-3IG level. [Pg.41]

In the isolated model calculations the ionic form is only slightly stabilized with respect to the neutral one by 3.13 kcal/mol. The stability of the ionic complex was greatly enhanced, when the external field has been added to the Fock operator and the difference in the energies of the ionic and neutral forms increased to about 50 kcal/mol in favour of the ionic complex. A comparison of the energies and charge distributions in the isolated and embedded clusters can be found in the Table 2 [224]. [Pg.41]

Alauddin M, Biswal HS, Gloaguen E, Mons M (2014) Intra-residue interactions in proteins interplay between serine or cysteine side chains and backbone conformations, revealed by laser spectroscopy of isolated model peptides. Phys Chem Chem Phys. doi 10.1039/ c4cp04449e... [Pg.265]

Fig. 13 Optimized geometries for two interacting NCs (model 2) with the 101/101, 101/001, 001/001 and 100/001 interfaces, along with the corresponding DOS (curves of different colors) compared to that of the isolated model 2 (red curves) calculated at the DFTB level of theory ( Fig. 13 Optimized geometries for two interacting NCs (model 2) with the 101/101, 101/001, 001/001 and 100/001 interfaces, along with the corresponding DOS (curves of different colors) compared to that of the isolated model 2 (red curves) calculated at the DFTB level of theory (<T = 0.18 eV). Reproduced from [188] by permission of The Royal Society of Chemistry (http // pubs.rsc.Org/en/content/articlelanding/2013/EE/C3EE24100A...
D. Fichou, G. Horowitz and F. Gamier, Polaron and Bipolaron formation on isolated model thiophene oligomers in solution, Synth. Met., 1990, 39, 125 D. Fichou, G. Horowitz, B. Xu and F. Gamier, Stoichiometric control of the successive generation of radical-cation and dication of extended alpha-conjugated oligothiophenes a quantitative model for doped polythiophene, Synth. Met., 1990, 39, 243. [Pg.314]


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See also in sourсe #XX -- [ Pg.150 , Pg.151 ]




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