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Activation stepladder

Figure 16, Stepladder simulation of (P/Z) falloff data for F-for-F activated CHgCF F (95), Input parameters , 0,17 eV E t, 4,0 eV /(Et) given by Equation 101 to 11,0 eV, Key to plot points ( ) experimental data ( ) calculated results. Figure 16, Stepladder simulation of (P/Z) falloff data for F-for-F activated CHgCF F (95), Input parameters <AEt>, 0,17 eV E t, 4,0 eV /(Et) given by Equation 101 to 11,0 eV, Key to plot points ( ) experimental data ( ) calculated results.
Figure 17. Stepladder simulation of (VIZ) falloff data for F-for-F activated CHfiF F ( ). Input parameters S.O eV others and... Figure 17. Stepladder simulation of (VIZ) falloff data for F-for-F activated CHfiF F ( ). Input parameters S.O eV others and...
A more carefully constructed approach to energy transfer explicitly accounts for the energy distribution of the chemically activated product (5,6,26,27), The initial distribution of energies upon production as well as the transient distributions formed by collisional relaxation of internal energy are used to calculate rate constants for imimolecular reaction. The formalism of Bunker (7,8,9) based on general RRKM theory is convenient for recoil chemical activation, since it explicitly accounts for both rotational and vibrational excitation in the product. In the cyclobutane model system reported, a stepladder approach to deactivation was incorporated, with the step size being a parameter determined by the best fit to the data (6). The overall processes considered are illustrated in Equation 4. [Pg.129]

Stepladder Modds.— Weak collision effects can, to a first approximation, be taken into account by using a sequence of single down steps instead of one down step for deactivation (see above). For chemical and also optical activation,... [Pg.194]

Whereas the relative variations of values for various collision partners are fairly certain, the absolute values can only be derived as reliably as the calculated k( ) used in the interpretation (see below). This disadvantage, as compared to low-pressure themud activation experiments, is compensated for by the possibility of producing higher excitation. With the high precisions obtainable today, some information on the functional form of the collisional transition probability has also been derived. Figure IS shows exponential and stepladder models for P(E IE)... [Pg.196]

As shown in this review, the properties of polyphenylene-based materials, so as to maximise their potential as active materials in LEDs or polymer lasers, can be controlled by dehberate synthetic design. By incorporating bridges between some or all of the phenylene units to make ladder or stepladder polymers the effective conjugation length of the polymer may be controlled, while the interactions between the chains and the injection of charges may be regulated by careful selection of substituents. By these means it is possible to minimise interchain interactions, which lead to loss of luminescence... [Pg.73]

Until now, it is virtually impossible to evaluate the function k(E, E ) for polyatomic molecules. For this reason, the theory of collisional activation and deactivation is to a considerable extent based on hypotheses concerning the general properties of the function k(E, E ). The two alternative hypotheses substantially simplifying the microscopic kinetic equations are the strong-collision hypothesis and that of stepladder activation and deactivation [336, 339, 486]. [Pg.97]

On the other hand, the stepladder mechanism of activation presupposes that one collision of AB with M causes a small change in the energy of AB, i.e. ((AE) ) (kT). In this case, relaxation is described by the diffusion equation... [Pg.97]

The non-equilibrium energy distribution function of molecules AB depends much more on the activation mechanism than the fall-off curve. The qualitative behaviour of the population ratio X(E)/X (E) for these two cases is shown in Fig. 25. For the strong-collision mechanism the depletion of population is seen to occur only for energy levels above Ea whereas for the stepladder mechanism it is below this level. [Pg.101]

Fig. 25. Non-equilibrium distribution function X(E) versus energy 1 stands for strong collisions, 2 for stepladder activation and deactivation. X (E) is the equilibrium distribution function, Ea the dissociation energy... Fig. 25. Non-equilibrium distribution function X(E) versus energy 1 stands for strong collisions, 2 for stepladder activation and deactivation. X (E) is the equilibrium distribution function, Ea the dissociation energy...
There is no provision in Subpart X that requires fall protection for an employee while working from a portable stepladder. However, if the employee will be on a surface prior to ascending or upon exiting the ladder for which another Subpart in 1926 requires fall protection, then fall protection would be required at such times. General requirements for fall protection can be found at Subpart M of 29 CFR Part 1926, while requirements specific to a particular activity or equipment can be found at its applicable Subpart in 29 CFR Part 1926. [Pg.441]


See other pages where Activation stepladder is mentioned: [Pg.177]    [Pg.194]    [Pg.195]    [Pg.196]    [Pg.3]    [Pg.117]    [Pg.176]    [Pg.102]    [Pg.168]    [Pg.39]    [Pg.369]   
See also in sourсe #XX -- [ Pg.97 ]




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