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Parameter 80 values, transition applications

Decreasing the diameter results in the decrease of the characteristic mixing time, which is the key to optimal conditions for fast processes, however, this favours a decrease of the effective coefficient of the turbulent diffusion The D,u, values form the lower limit, using geometrical parameters, for the application of tubular turbulent devices under industrial production conditions. Calculations demonstrate, that at < 0.023 m, = 4 m/s, and y= 45° the diffusion coefficient value does not exceed 10 m /s, which is typical for the transition flow mode in cylindrical channels. [Pg.46]

The exact results shown in previous paragraphs are obtained by using the analytical calculation under the hypothesis that the transition rate matrix M of Markov process is available. But in practical application, this assumption is not always true. Assume now that the M is unknown and that only available data are a single sample path of Markov process. Since the realistic data set of this trajectory is not available here, it need to be simulated with parameter values given in Table 1. The goal is to use the perturbation analysis technique to estimate the DlM s measures mentioned above from this data set. In fact, the simulation is made for 100000 transitions. [Pg.954]

We first consider the region of parameter values between the ignition and extinction points 6 and 6 (Fig. 4). We assume that the system is initially on the lower branch and inquire about the average time needed to undergo a spontaneous explosion in the form of a jump across the unstable state branch. A straightforward application of expression (15) in which the specific structure of the potential, eq. (21b), is taken into account, leads to the results summarized in Fig. 7. As expected, the transition time tends to zero as the system approaches the ignition point. Otherwise, the transition times are extraordinarily large, unless one deals with a small size system or, alternatively, with localized fluctuations in a sufficiently small volume. It seems therefore... [Pg.195]

The ° mn coefficients are the mean values of the generalized spherical harmonics calculated over the distribution of orientation and are called order parameters. These are the quantities that are measurable experimentally and their determination allows the evaluation of the degree of molecular orientation. Since the different characterization techniques are sensitive to specific energy transitions and/or involve different physical processes, each technique allows the determination of certain D mn parameters as described in the following sections. These techniques often provide information about the orientation of a certain physical quantity (a vector or a tensor) linked to the molecules and not directly to that of the structural unit itself. To convert the distribution of orientation of the measured physical quantity into that of the structural unit, the Legendre addition theorem should be used [1,2]. An example of its application is given for IR spectroscopy in Section 4. [Pg.298]

There exists no significant comprehensive fit of spectral data of H2 with which we might here make comparison. Our discussion above demonstrates that, as for GaH above, application of an algorithm based on Dunham s algebraic approach to analysis of vibration-rotational spectral data of H2, especially through implementation of hypervirial perturbation theory [30,72] that allows the term for the vibrational g factor in the hamiltonian in formula 29 to be treated directly in that form, proves extremely powerful to derive values of fitting parameters that not only have intrinsic value in reproducing experimental data of wave numbers of transitions but also relate to other theoretical and experimental quantities. [Pg.291]

Although the statistical mechanical theories such as those described above yield exact analytic expressions for various quantities characterizing the conformation of an interrupted helix, those expressions are so complicated that it is of both theoretical and practical value to simplify them, with the imposition of suitable restrictions on parameters, to forms that are amenable to straightforward computations and also, hopefully, to direct comparisons with observed data. Various attempts have been made, and they are summarized in Poland-Scheraga s book (10). Though not available at the time this book was published, the approximations worked out by Okita et al. (13) are of great practical use for their wide applicability and simplicity. Their method is described below in some detail, because it has been consistently used in our statistical-thermodynamic analyses of helix-coil transition phenomena. [Pg.73]

Applications to Small Molecules. - 2.2.1 Intensity of Half-field Transition or Resolved Dipolar Splitting. In the pH range 8-10 the dominant species in solutions of Cu(II) and 2,2 -bipyridine (bpy) is [Cu(bpy)(OH)]22+.30 Well-resolved EPR spectra were obtained. The value of the zero-field splitting parameter D and the relative intensity of the half-field transition gave r = 3.4 A. [Pg.321]


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See also in sourсe #XX -- [ Pg.372 , Pg.373 , Pg.374 , Pg.375 , Pg.376 , Pg.377 , Pg.378 , Pg.381 ]




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Application Parameters

Parameter 80 values, transition

Parameter value

Transition applications

Transition parameters

Transitional value

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