Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Relaxation limits

Fig. 17.3. Creep is important in (our classes of design (a) displacement-limited, (b) failure-limited, (c) relaxation-limited and (d) buckling-limited. Fig. 17.3. Creep is important in (our classes of design (a) displacement-limited, (b) failure-limited, (c) relaxation-limited and (d) buckling-limited.
Computation of Mossbauer Spectra in Slow and Fast Relaxation Limit... [Pg.127]

The halo globular cluster system also provides valuable information, since accurate distances, and hence reliable ages, can be derived. Mackey Gilmore (2004) recently acquired and compiled a new, nearly complete, internally consistent set of photometric studies of the globular cluster population in both the Milky Way and its satellite galaxies they deduce, from analysis of HB morphol-ogy, age, abundance and structural information, somewhat more relaxed limits... [Pg.245]

In practice, it is also possible to take advantage of the closeness of these rate constants to their relaxation limit and interpolate/extrapolate values from a correlation between deprotonation rate constants and pATas. The rate constants for such a correlation come from measurements for secondary or... [Pg.36]

These points have been pursued in detail for two reasons. The first is to indicate the level of uncertainty in deriving pATas when the rate of deprotonation falls significantly short of its relaxation limit and the structure-reactivity correlation for the alkene conjugate base of the cation is insufficiently defined. The second is that the identity of the rate constants for 2-propene and 2-butene still imply a difference of 0.3 log units between 2-propyl and 2-butyl cations. In so far as this difference corresponds with the small difference in geminal interaction of the OH groups, the implication is that as measured by their HIAs the two ions have the same stability (cf. discussion on p. 25). In conclusion, the preferred pATR for the 2-propyl cation is listed below with the more secure values for the /-butyl and ethyl cations. [Pg.48]

It is not intended to extend this discussion of reactions of carbocations with water to consideration of the alcoholic solvents trifluoroethanol (TFE) and hexa-fluoroisopropanol (HFIP), which have been extensively studied and reviewed by McClelland and Steenken.3 However, an important point of interest of these solvents is that their reactivities toward carbocations are greatly reduced compared with water (by up to a factor of 104 in TFE and 108 in HFIP) and that differences in rate constants can be observed between cations which would react indiscriminately at the solvent relaxation limit in water. The following comparisons of rate constants for carbocations with similar pAR values reacting with hexafluoroiso-propanol241,242 reinforces the conclusion that structural variations in the cation lead to changes in intrinsic barrier and, for example, that phenyl substitution is probably associated with such an increase in going from benzyl to benzhydryl (although the benzyl cation itself is not shown). [Pg.85]

Boltzmann factor) of finding the atom in the respective state. In the fast relaxation limit, the nucleus senses the average spin (actually the average Bint), obtained by thermally averaging the expectation values of the individual level, in the present case (Sz)th = SZ) +1/2 + + e AEIkT), where AE = g/ B is the Zeeman... [Pg.45]

Ramasesha et al.216) introduce a coupling between the HS and LS electronic states via lattice strain to take care of the appearance of residual paramagnetism at low temperatures. The resultant mixing of these states is a contradiction to the observations of Mossbauer measurements where the HS and LS states appear separately (slow relaxation limit). Moreover, this mixing cannot occur in the framework of ligand field theory. [Pg.179]

Relaxation limit of a chemical oscillator) Analyze the model for the chlorine dioxide-iodine-malonic acid oscillator, (8.3.4), (8.3.5), in the limit b i. Sketch the limit cycle in the phase plane and estimate its period. [Pg.291]

The Lindemann model discussed above provides the simplest framework for analyzing the dynamical effect of thermal relaxation on chemical reactions. We will see that similar reasoning applies to the more elaborate models discussed below, and that the resulting phenomenology is, to a large extent, qualitatively the same. In particular, the Transition State Theory (TST) of chemical reactions, discussed in the next section, is in fact a generalization of the fast thermal relaxation limit of the Lindemann model. [Pg.488]

The second form of relaxation is called spin-spin relaxation. This form involves any change in the quantum state of the spin. Thus, any of the transitions shown in Figure 3.1 can cause spin-spin relaxation. In particular, the exchange of magnetization between spins via a zero quantum transition is a very effective mechanism for spin-spin relaxation. Thus, spin-spin relaxation is analogous to fluorescence energy transfer. Because spin-spin relaxation limits the lifetime of the excited state, it affects the line width of the observed resonance lines due to the uncertainty principle shortlived states have ill-defined frequencies. The actual relationship between the spin-spin relaxation rate and the line width (Av) is given by R2, the rate of spin-spin relaxation T2 is the time constant for spin-spin relaxation,... [Pg.45]

This corresponds to fully relaxed emission coming from the equilibrated distribution of vibronic states. Equation (121) thus interpolates between the previous expression, Eq. (84), which contains no VR, and the fast relaxation limit, Eq. (129), whereby the emission is fully relaxed. The key parameter controlling this behavior is yVb/yr. [Pg.215]

I2J. The Tm ion can give blue emission, but cross-relaxation limits the activator concentration, so that saturation occurs. In spite of its saturation at high excitation densities, the old ZnS Ag has not yet been surpassed under these conditions. As a consequence the screen brightness is limited by the blue-emitting phosphor. Extensive research by many laboratories has not changed this situation. [Pg.143]

The so-called fast relaxation limit in which coe cog. In this case the structural relaxation gives rise to a broad backgroimd scattering in the frequency scale, leaving the Rayleigh-Brillouin spectrum nearly unchanged. [Pg.493]


See other pages where Relaxation limits is mentioned: [Pg.173]    [Pg.505]    [Pg.505]    [Pg.139]    [Pg.152]    [Pg.319]    [Pg.217]    [Pg.266]    [Pg.366]    [Pg.36]    [Pg.47]    [Pg.51]    [Pg.72]    [Pg.103]    [Pg.210]    [Pg.44]    [Pg.45]    [Pg.176]    [Pg.194]    [Pg.335]    [Pg.135]    [Pg.140]    [Pg.98]    [Pg.210]    [Pg.500]    [Pg.484]    [Pg.487]    [Pg.792]    [Pg.263]    [Pg.156]    [Pg.391]   
See also in sourсe #XX -- [ Pg.291 ]




SEARCH



© 2024 chempedia.info