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Well depths, determination

If the energy of the transition state is known, the activation energy from the well to the transition state can be determined if the well depth is known. In many cases, the equilibrium has been measured in others, the well depth can be estimated fairly accurately. The rate of the reaction is not dependent on the well depth, so that the depth cannot be determined by studying the kinetics at low pressure. The well depth determines the lifetime of the complex, but this depth does not affect the reaction efficiency. [Pg.31]

A different approach is that based on the density-functional Gordon-Kim method [222], which has been used to calculate the interaction of Ar over an Ar substrate [223] and for rare gases on graphite [150,151]. It permits one to take into account the non-two-body additive effects and to give indications about the choice of the suitable effective parameters. The well depths determined by Freeman [151] in that theoretical development are substantially lower than those found by other methods. Nevertheless, the disagreement is due, in part, to the uncertainties and approximations in the theoretical calculations. [Pg.461]

The two-dimensional interaction potential of the N2(X Sg)-He(X S) system was obtained from highly correlated ab initio MCSCF-CI calculations. The well depth, determined to be about 140 cm (0.017 eV), confirms a possible bound HeN ion. The well depth... [Pg.3]

A measurement procedure has been developed that allows to determine the mass of the inclusions as well as their locations with respect to radius, angle, and depth (2). For the depth determination use is made of the approximate 1/R dependence of the magnetic field strength from the distance R to the inclusion When in a first measurement at a small lift off an inclusion is detected, the measurement is repeated at an increased lift off From the signal ratio the depth can be calculated or seen from a diagram like fig. 5a which was generated experimentally. After that, from calibration curves like fig. 5b the absolute value of the signal leads to the mass of the inclusion. [Pg.989]

It is of interest to note that in this model the anisotropy in the attractive energy is determined by the same parameter, 7, as that controlling the anisotropy in the repulsive energy. In these expressions for the contact distance and the well depth their angular variation is contained in the three scalar products Uj Uj, Uj f and uj f which are simply the cosines of the angle between the symmetry axes of the two molecules and the angles between each molecule and the intermolecular vector. [Pg.69]

When the well depth or diameter is unknown or a water-level measurement is not possible, purging should be carried out by pumping the well for a pre-determined period of time (e.g., at least 30min). Measurement of groundwater parameters should be monitored at intervals during the purging process and at the time of sample collection (Figure 3). [Pg.804]

For consistency, an initial well associated with the formation of an adduct of the metal ion with the alkane should be included in Figure 11. The chemical activation associated with the formation of such an adduct is likely to be essential in overcoming intrinsic barriers associated with insertion into C-H bonds. In comparison to larger hydrocarbons, the weaker interaction of ethane with first row group 8-10 metal ions may be insufficient to overcome intrinsic barriers for insertion. This would explain the failure to observe dehydrogenation of ethane by these metal ions, even though the process is known to be exothermic. The well depths could be determined from high pressure equilibria. Studies in our laboratory and elsewhere have indicated the ease with which many of... [Pg.34]

This potential was developed to ensure that the molecules inside the sphere never escape and maintain a fully solvated system during molecular dynamics. Here, es, Rs, ew and Rw are the van der Waals constants for the solvent and the wall and rj is the distance between the molecule i and the center of the water sphere, Ro is the radius of the sphere. The quantities A, B and Rb are determined by imposing the condition that W and dW/dr, vanish at r, = Ro. The restraining potential W is set to zero for r, < R0. The van der Waals parameters Es, ew, Rs and Rw can also be specifically defined for different solvents. The constants Awaii and Cwan are computed using a well depth of es = ew = 0.1 kcal and the radius of Rs = Rw = 1.25 A. For the other set of simulations, especially for the hydride ion transfer, we applied periodic boundary conditions by using a spherical boundary shell of 10.0 A of TIP3P40 water to cover the edges of the protein. [Pg.263]

We do need to determine the well depth, however, in order to evaluate the absolute barrier height. The well depth corresponds to AH° for the reaction... [Pg.91]

Monitoring the well for leaks and nearby aquifers for contamination must also be considered. The extent of monitoring will vary based on the applicable environmental regulations and nearby potable aquifers. Monitoring wells can be constructed to monitor shallow or deep aquifers, and the cost of a these wells is determined by the required depth and the geology of the site. Additional costs include ancillary surface equipment and alarm systems (Mickley 2006). [Pg.44]

The aim of the present study is to investigate the validity of the pairwise additivity of two-body and three-body potentials for He2Br2. These results are compared with ah initio calculations" and a simple model of the three-body potential is proposed to determine well depths and equilibrium structures for different isomeric configurations of the complex, as well as the minimum energy pathways through them. Additionally, variational methods are used to calculate the vibrational states of He2Br2. The wavefunctions of the lower states are analyzed in terms of probability distributions of the internal coordinates and the zero-point energy of the vdW cluster is evaluated. [Pg.349]

The values of ev and ay are the well depth and size parameters, respectively, for the two interacting atoms i and j. In the case that one of the interacting atoms is a zeolite atom and the other is a sorbate atom, the cross terms ezeo-sorb and o-zeo-Sorb are determined from the Lorentz-Berthelot combination rules (7). When polarization interactions are accounted for, such as those between adsorbates and zeolite extra framework cations, Eq. (2) is written in the form... [Pg.8]

From the functional form of Eq. 12.5, it is easy to see that as distance between the molecules rjj becomes small, the potential becomes very repulsive due to the dominance of the first term (r 12 dependence). However, the repulsive term drops off very rapidly with distance, and the attractive term dominates at long distances. The interaction potential has a minimum at some intermediate distance, with a characteristic attractive well-depth. The parameter oij represents a net collision diameter, and etj determines the depth (strength) of the interaction. Methods for obtaining these parameters from experiment and other estimation techniques are discussed in Section 12.2.3. Combining rules to estimate the parameters interactions between unlike molecules are given in Section 12.2.4. [Pg.492]

The first maximum of Ai2(z) lies at z = 1.018, and at z = 0 it has decreased to 44% of its value at the first maximum. In a measured distribution, therefore, the 44% value at the low-energy side of the low-energy peak determines the position of from which by relation (II.6) the well depth > of K (R) can be obtained. The measured energy difference between the peak position ep and e, allows determination of the constant c by... [Pg.419]

A quantitative evaluation of a measured energy dependence of the ratio has been made only for the system He(23S)-Ar for which V R) and T(fl) are known, so that the evaluation leads to a determination of parameters of V+(R). In classical model calculations,43 using a semiempirically determined potential V+(R)1] that only slightly deviates from the one determined from elastic scattering30 and r( ) = 4000 exp(-R/0.36) (au), which was determined by the requirements that the total ionization cross-section curve due to Pesnelle et al.43 be reproduced with the chosen K (R), for a Morse potential V+(R) the following parameter values were determined well depth 16 meV, equilibrium distance 5.67a0, and shape... [Pg.453]

Associative ionization was also observed between atoms in Sr 5snt states and the ground Sr 5s2 state in a beam of Sr by Worden et al.98 They used multi step resonant laser excitation of the Sr 5sn states, and at Sr number densities of 1013 cm 3, they observed Sr2+. They were able to determine the well depth of Sr2+ to be 0.77 eV. [Pg.240]

Results. The first explosive fracturing test detonated 100 qt of NG1 displaced into the formation from well 3 at a depth interval from 70 to 74 ft. Following detonations in wells 3 and 4, fracture intervals in the wellbores connecting the injection well 3 and other wells were determined by airflow measuerments. [Pg.107]

The shape of the well is determined solely by the heavy nuclei and the distance between them62. Where the hydrogen atom spends its time is determined by the depths of the wells and the height of the barrier between them. The 2H isotope sits deeper within a particular well than does H and the 3H isotope deeper still. [Pg.165]


See other pages where Well depths, determination is mentioned: [Pg.228]    [Pg.243]    [Pg.10]    [Pg.919]    [Pg.70]    [Pg.92]    [Pg.96]    [Pg.101]    [Pg.123]    [Pg.799]    [Pg.26]    [Pg.130]    [Pg.76]    [Pg.91]    [Pg.51]    [Pg.242]    [Pg.17]    [Pg.738]    [Pg.424]    [Pg.440]    [Pg.454]    [Pg.456]    [Pg.533]    [Pg.32]    [Pg.135]    [Pg.66]    [Pg.147]    [Pg.68]    [Pg.107]    [Pg.827]    [Pg.321]    [Pg.323]   
See also in sourсe #XX -- [ Pg.461 ]




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