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Canonical mechanism

The change in the nature of the tetrazole substrate on going from tetrazolide 7 to contact ion pairs, solvent-separated ion pairs with a metal cation, to complexes of 231 and 232 type, etc., can result in deviations from the canonical mechanisms like those described above (Schemes 22 and 23). Also, the possibility cannot be excluded that the ion pairs formed by anion 7 react with the electrophile concurrently by several alternative pathways. We believe that just this versatility of reaction routes explains the difference between the predicted rate and selectivity of the electrophilic attack under ideal conditions and the experimental result. In the light of these comments, new data on the application of ion pairs formed by anions of type 7 to the synthesis of N-substituted tetrazoles are discussed. As far as possible, attention is given to conclusions with respect to the regioselectivity of electrophile attack. [Pg.321]

Canonical mechanism kunitz- and kazal-type inhibitors... [Pg.1709]

Although one can write a canonical mechanism for retaining O-glycosidases, there are departures from this mechanism in acid-catalytic machinery and the nature of the nucleophile (for some families, not the carboxylate shown). In Table 5.4 are set out the nature of the catalytic groups, the protonation trajectory and the conformations of substrate and glycosyl enzyme, where at least two of these are known. [Pg.372]

Figure 5.32 Canonical mechanism for a retaining glycosidase or transglycosylase Whether the substrates are pyranosidases or furanosidases, whether the leaving group is axial or equatorial and whether the protonation trajectory is syn or anti depend on the enzyme. If R = R, then the principle of microscopic reversibility requires transition states 1 and 2 to be identical. More generally, the group which acts as a general acid in the first step must act as a general base in the second. Figure 5.32 Canonical mechanism for a retaining glycosidase or transglycosylase Whether the substrates are pyranosidases or furanosidases, whether the leaving group is axial or equatorial and whether the protonation trajectory is syn or anti depend on the enzyme. If R = R, then the principle of microscopic reversibility requires transition states 1 and 2 to be identical. More generally, the group which acts as a general acid in the first step must act as a general base in the second.
The canonical mechanism shown in Figure 5.32 requires the same carboxylate group which acts as a general acid in the first step to act as a general base in the second. Its pAa must, therefore, decrease between the free enzyme and the glycosyl-enzyme intermediate. Direct NMR observation of active site carboxy-lates in the GH 11 p-xylanase of B. circulans already discussed in Section 5.4.2 indicated that the acid-base catalytic Glu 172 had a (microscopic) pAa of 6.7 in the free enzyme and 4.2 in the 2-deoxy-2-fluoro-a-xylobiosyl enzyme generated from the Withers inactivator 2,4-dinitrophenyl 2 -deoxy-2 -fluoro-p-xylobioside. ... [Pg.387]

Figure 5.53 Canonical mechanism for inverting glycosyl transferases. A divalent metal ion is shown acting as an electrophilic catalysts however, data for GT63 (B fold) suggest that any metal-ion dependence of B-fold enzymes arises from metal-promoted product release, not catalysis and metals are rare in transferases with the GTB fold. Figure 5.53 Canonical mechanism for inverting glycosyl transferases. A divalent metal ion is shown acting as an electrophilic catalysts however, data for GT63 (B fold) suggest that any metal-ion dependence of B-fold enzymes arises from metal-promoted product release, not catalysis and metals are rare in transferases with the GTB fold.
It is generally thought that these four canonical mechanisms of IgE-mediated activation of human FceRI + cells are responsible for the pathophysiological involvement of these cells in the majority of patients with allergic disorders [34], However, there is evidence that a significant percentage of allergic diseases (e.g. certain cases of intrinsic asthma and chronic idiopathic urticaria) cannot be explained by the four classical mechanisms of FceRI + cell activation. [Pg.63]

The two canonical mechanisms of enzymatic glycoside hydrolysis were first proposed by Koshland in 1953. Since then, considerable amounts of structural and mechanistic data have been accumulated in support of the proposed mechanisms, both of which involve nucleophilic displacement steps. The reactions result in either net (1) inversion, or (2) retention of the substrate anomeric configuration." " " The following section provides an account of these two basic mechanistic groups of enzymes. [Pg.391]

This example also shows that the canonic mechanism is not the simplest one and it is not minimal in any sense (although it is unique). Its major advantage is that it can quickly be constructed and by an algorithm. [Pg.66]

Here we describe three canonical mechanisms that seem most relevant to the study of MEPs ... [Pg.777]

The grand canonical ensemble is a set of systems each with the same volume V, the same temperature T and the same chemical potential p (or if there is more than one substance present, the same set of p. s). This corresponds to a set of systems separated by diathennic and penneable walls and allowed to equilibrate. In classical thennodynamics, the appropriate fimction for fixed p, V, and Tis the productpV(see equation (A2.1.3 7)1 and statistical mechanics relates pV directly to the grand canonical partition function... [Pg.375]

In addition, there could be a mechanical or electromagnetic interaction of a system with an external entity which may do work on an otherwise isolated system. Such a contact with a work source can be represented by the Hamiltonian U p, q, x) where x is the coordinate (for example, the position of a piston in a box containing a gas, or the magnetic moment if an external magnetic field is present, or the electric dipole moment in the presence of an external electric field) describing the interaction between the system and the external work source. Then the force, canonically conjugate to x, which the system exerts on the outside world is... [Pg.395]

Consider two systems in thennal contact as discussed above. Let the system II (with volume and particles N ) correspond to a reservoir R which is much larger than the system I (with volume F and particles N) of interest. In order to find the canonical ensemble distribution one needs to obtain the probability that the system I is in a specific microstate v which has an energy E, . When the system is in this microstate, the reservoir will have the energy E = Ej.- E due to the constraint that the total energy of the isolated composite system H-II is fixed and denoted by Ej, but the reservoir can be in any one of the R( r possible states that the mechanics within the reservoir dictates. Given that the microstate of the system of... [Pg.395]

The above derivation leads to the identification of the canonical ensemble density distribution. More generally, consider a system with volume V andA particles of type A, particles of type B, etc., such that N = Nj + Ag +. . ., and let the system be in themial equilibrium with a much larger heat reservoir at temperature T. Then if fis tlie system Hamiltonian, the canonical distribution is (quantum mechanically)... [Pg.397]

If one denotes the averages over a canonical distribution by (.. . ), then the relation A = U-T S and U = (W) leads to the statistical mechanical coimection to the themiodynamic free energy A ... [Pg.398]

The T-P ensemble distribution is obtained in a maimer similar to the grand canonical distribution as (quantum mechanically)... [Pg.417]

No system is exactly unifomi even a crystal lattice will have fluctuations in density, and even the Ising model must pemiit fluctuations in the configuration of spins around a given spin. Moreover, even the classical treatment allows for fluctuations the statistical mechanics of the grand canonical ensemble yields an exact relation between the isothemial compressibility K j,and the number of molecules Ain volume V ... [Pg.647]

Quack M 1984 On the mechanism of reversible unimolecular reactions and the canonical ( high pressure ) limit of the rate coefficient at low pressures Ber. Bunsenges. Phys. Chem. 88 94-100... [Pg.794]

As reactants transfonn to products in a chemical reaction, reactant bonds are broken and refomied for the products. Different theoretical models are used to describe this process ranging from time-dependent classical or quantum dynamics [1,2], in which the motions of individual atoms are propagated, to models based on the postidates of statistical mechanics [3], The validity of the latter models depends on whether statistical mechanical treatments represent the actual nature of the atomic motions during the chemical reaction. Such a statistical mechanical description has been widely used in imimolecular kinetics [4] and appears to be an accurate model for many reactions. It is particularly instructive to discuss statistical models for unimolecular reactions, since the model may be fomuilated at the elementary microcanonical level and then averaged to obtain the canonical model. [Pg.1006]

Figure Bl.16.14. Top, the canonical axes for triplet naphthalene. The z-axis is directed out of the plane of the paper. Bottom, energy levels and relative populations during the CIDEP triplet mechanism process. See text... Figure Bl.16.14. Top, the canonical axes for triplet naphthalene. The z-axis is directed out of the plane of the paper. Bottom, energy levels and relative populations during the CIDEP triplet mechanism process. See text...
Statistical mechanics may be used to derive practical microscopic fomuilae for themiodynamic quantities. A well-known example is tire virial expression for the pressure, easily derived by scaling the atomic coordinates in the canonical ensemble partition fiinction... [Pg.2248]

Chesnut D A and Salsburg Z W 1963 Monte Carlo procedure for statistical mechanical calculation in a grand canonical ensemble of lattice systems J. Chem. Phys. 38 2861-75... [Pg.2280]

The canonical ensemble is the name given to an ensemble for constant temperature, number of particles and volume. For our purposes Jf can be considered the same as the total energy, (p r ), which equals the sum of the kinetic energy (jT(p )) of the system, which depends upon the momenta of the particles, and the potential energy (T (r )), which depends upon tlie positions. The factor N arises from the indistinguishability of the particles and the factor is required to ensure that the partition function is equal to the quantum mechanical result for a particle in a box. A short discussion of some of the key results of statistical mechanics is provided in Appendix 6.1 and further details can be found in standard textbooks. [Pg.319]


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