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Potential energy difference

The laser intensities are taken to be the possible lowest. The intensity in case (b) is almost three times larger than the others. This is simply due to the fact that the transition dipole moment exponentially decays from the equilibrium position and also the potential energy difference increases. Note again that the coordinate-dependent level approximation works well. In order to demonstrate the selectivity the time evolution of the wave packets on the excited state are shown in Fig 41. As a measure of the selectivity, we have calculated the target yield by... [Pg.170]

All of these one- and two-body models have assumed hard walls for the box (potential V = 00 for r > R). The actual potential energy difference between the lower edge of the conduction band of the macrocrystal and the vacuum level amounts to 3.8 eV. This potential dqpth was used in the quantum mechanical calculation of curve b. It is seen that the energy lowering is substantial, particularly at small diameters. [Pg.173]

Table 3-1. Calculated potential and free energy differences for path B (in kcal/mol) between the determined structure and the reactant (ES complex), where Ait is the total HF potential energy difference, A Eqm refers to the QM energy difference between two QM subsystems. A 1 qm/MM is the free energy change in the QM/MM interaction, and A F = AEqm + A I qm/MM- Numbers without parentheses correspond to the present work and numbers in parentheses correspond to our previous determinations (path D) [33]... Table 3-1. Calculated potential and free energy differences for path B (in kcal/mol) between the determined structure and the reactant (ES complex), where Ait is the total HF potential energy difference, A Eqm refers to the QM energy difference between two QM subsystems. A 1 qm/MM is the free energy change in the QM/MM interaction, and A F = AEqm + A I qm/MM- Numbers without parentheses correspond to the present work and numbers in parentheses correspond to our previous determinations (path D) [33]...
In this equation, we used the fact that the potential energy difference between the states Aj, or A + AX, and state A + A /2 is equal to AUiyi+1/2, which is a consequence of the linear form of (2.42). [Pg.61]

UU is the Hamiltonian difference (the perturbation) the angle brackets represent a canonical ensemble average performed on an equilibrated system designated by the subscript. Usually the kinetic component of the Hamiltonian is not included in the free energy calculation, and A- //, n can be replaced by the potential energy difference AU = Ui - U0. [Pg.203]

Fig. 16. Three dimensional conformational map of cyclohexane. The representation is analogous to that of Fig. 15 the third (vertical) coordinate is the potential energy. The given calculated potential energy differences (kcal mole-1) of the minima and transition states are drawn to scale. The interconnecting curves are drawn qualitatively they are merely meant to indicate the absence of intermediate further minima and maxima. See ref. 106 for details of analytical representations of conformational maps of cyclohexane... Fig. 16. Three dimensional conformational map of cyclohexane. The representation is analogous to that of Fig. 15 the third (vertical) coordinate is the potential energy. The given calculated potential energy differences (kcal mole-1) of the minima and transition states are drawn to scale. The interconnecting curves are drawn qualitatively they are merely meant to indicate the absence of intermediate further minima and maxima. See ref. 106 for details of analytical representations of conformational maps of cyclohexane...
Therefore the vacuum potential energy difference is given by... [Pg.163]

A special class of reservoir capacity known as extraction was introduced in Chapter 4. Thermodynamically, the process is no different from the features described above, but from a use point of view, the process represents a special kind of bottle. Instead of leakage via diffusion caused by a potential energy difference, the leak arises from a shift in the partition coefficient from a change in temperature or in the solvent environment. [Pg.102]

Molecular specificity is afforded by control of the potential energy difference across the electrode-solution interface. The selectivity or resolution of electrochemistry is not nearly as great as we would like, and the inability to distinguish between two or more species can be a serious weakness. Solution electrochemistry suffers by comparison with mass spectrometry in the same sense that optical spectra in solution suffer by comparison with vapor-phase spectra. [Pg.4]

So it is also possible to use the form (139) for the vacuum charge current density, a form that eliminates any geometric unit such as Ar that is not fully relativistic. However, A is, strictly speaking, a potential energy difference and not a field. [Pg.28]


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See also in sourсe #XX -- [ Pg.99 , Pg.100 ]




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Definitions and Approximations Associated with Different Types of Potential Energy Curves

Difference mass spectrum, potential energy

Difference potential

Energy differences

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