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Higher-order complexes

To conclude, the introduction of species-selective membranes into the simulation box results in the osmotic equilibrium between a part of the system containing the products of association and a part in which only a one-component Lennard-Jones fluid is present. The density of the fluid in the nonreactive part of the system is lower than in the reactive part, at osmotic equilibrium. This makes the calculations of the chemical potential efficient. The quahty of the results is similar to those from the grand canonical Monte Carlo simulation. The method is neither restricted to dimerization nor to spherically symmetric associative interactions. Even in the presence of higher-order complexes in large amounts, the proposed approach remains successful. [Pg.237]

B. Stabilization of Multiple Conformers of Higher Order Complexes ... [Pg.396]

The experimental results on He2 ICl and He2 Br2 demonstrate that by varying the expansion conditions it is possible to manipulate the relative abundances of the higher order complexes and drive the ground-state population to the more energetically stable configuration. The stabilization of multiple Rg XY conformers suggests that the influence of the multibody interactions... [Pg.397]

The association rate constants were the same within experimental error. The dissociation rate constant for 31 was however an order of magnitude larger than that for 32. The association rate constants determined with fluorescence correlation spectroscopy were similar to the rate constants determined using temperature jump experiments (see above). However, a significant difference was observed for the dissociation rate constants where, for the 1 1 complex, values of 2.6 x 104 and 1.5 x 104s 1 were determined in the temperature jump experiments for 31 and 32, respectively.181,182 The reasons for this difference were not discussed by the authors of the study with fluorescence correlation spectroscopy. One possibility is that the technique is not sensitive enough to detect the presence of higher-order complexes, such as the 1 2 (31 CD) complex observed in the temperature jump experiments. One other possibility is the fact that the temperature jump experiments were performed in the presence of 1.0 M NaCl. [Pg.213]

Protein-DNA complexes are usually formed by adding small portions of the protein solution to the DNA. The formation of the complex is best monitored by observing the changes of the DNA imino proton signals in a ID spectrum after each step. A reversed approach, i.e. adding the DNA to a protein solution, is not recommended because of the formation of higher order complexes by nonselective binding of protein to DNA. [Pg.122]

ATP-dependent proteases are complex proteolytic machines. They are present in eubacteria, archaebacteria, in eukaryotic organelles and, as the 20S or 26S proteasome, in the eukaryotic cytosol and nucleoplasm. The activators of all known ATP-dependent proteases are related. They all contain an AAA(+) ATPase domain as a module (Neuwald et al. 1999) and are thought to assemble into hexameric particles or, in the case of 26S proteasomes, are present in six variants in the 19S activators (Glickman et al. 1999). Like the ATPases, the proteolytic components of the ATP-dependent proteases form higher order complexes, but unlike for the ATPases, the symmetry of the protease assemblies varies, and the folds of the subunits need not be related. ClpP is a serine protease, FtsH a metalloprotease, and HslV and the proteasomes from archaebacteria and eubacteria are threomne proteases. [Pg.248]

A smaller secondary microscopic association constant compared to the first binding constant (k, = k2 > k2, = kl2) results in anticooperative binding behavior in cases A and B. If k, = k2 < k2i = kl2, as in cases D and E, the cooperative binding yields a higher amount of higher-order complexes. [Pg.46]

If micelles are very small, they can t regarded as a separate phase and the aggregates between substrate and surfactants are better described as higher-order complexes. [Pg.55]

AuCl2- or even a higher order complex. While it is possible that the enhanced capacity of Au1 for complexation with soft ligands may account for the disparate distributions of Ag and Au, fractionation of Au and Ag may also be caused by a significant Aum chemistry in seawater. The major species of Au111 in seawater are expected to be Au(OH)3 or Au(OH)3C1 (Baes and Mesmer, 1976). Although the analysis ofTumer etal. (1981) indicated that the field of Aum stability is somewhat outside the oxidation-reduction conditions encountered in seawater, a paucity of direct formation-constant observations for both Aum and Au1 creates substantial uncertainties. Furthermore, with respect to thermodynamic predictions of oxidation-reduction behaviour the ocean is not a system at equilibrium. [Pg.340]

The site selectivity switch, that is the site to which BF3 coordinated carbonyl rearrangement occurs, in the skeletal rearrangements of cyclobutene-fused diarylhomoben-zoquinones (43) is reported to result from higher order complexation. Thermodynamic... [Pg.453]

Plotting ([S]T - [S]0)/[CD]X vs. [CD]X gives the first estimated values for K1 1 and K1 2 from the intercept and the slope, respectively. The estimated values are substituted to Equation (3.134) to determine [CD], The stability constants are estimated after substituting the estimated [CD] values. Three or four iterations, after the first estimated values of K, K12, and [CD] are calculated from Equation (3.135) and Equation (3.133), yield constant values for the stability constants. However, the determination of the stability constants for higher order complexes is not possible with this approach. [Pg.183]

Fig. 3.2. A schematic representation of the molecular imprinting pre-arrangement phase (corresponding to 2 in Fig. 3.1), here using ()-nicotine as the template and carboxylic acid containing functional monomers. In this case a total of five states of complexation are proposed I, non-complexed template II, weak single point interaction III, strong single point interaction IV, combination of weak and strong interactions V, higher order complexes e.g. monomer interactions with template-template self-association complexes, higher monomer solvation levels. Fig. 3.2. A schematic representation of the molecular imprinting pre-arrangement phase (corresponding to 2 in Fig. 3.1), here using ()-nicotine as the template and carboxylic acid containing functional monomers. In this case a total of five states of complexation are proposed I, non-complexed template II, weak single point interaction III, strong single point interaction IV, combination of weak and strong interactions V, higher order complexes e.g. monomer interactions with template-template self-association complexes, higher monomer solvation levels.
Therefore, both K p and Kn can be evaluated from a plot of [A]t versus l/[B]r- If there are no higher order complexes in solution, this plot is linear with slope = K p and intercept = KuK p under the conditions KiiK p < [B]r. [Pg.625]

One difference in complexation performance of ionic versus neutral CDs is in their inability to participate in 1 2 or 1 3 complexations. The ionically charged CDs do not effectively form higher order complexes probably due to electrostatic repulsions between the first CD to sequester the drug and the incoming ionic CD. As the charge density increases, this repulsive effect is magnified. Rajewski et al. demonstrated that as the charge density of the SBE-p-CD increases from one to four to seven, the solubilization of cholesterol decreases. [Pg.678]


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See also in sourсe #XX -- [ Pg.7 ]




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