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Force constants for

To obtain the force constant for constructing the equation of motion of the nuclear motion in the second-order perturbation, we need to know about the excited states, too. With the minimal basis set, the only excited-state spatial orbital for one electron is... [Pg.439]

Determination of the paiameters entering the model Hamiltonian for handling the R-T effect (quadratic force constant for the mean potential and the Renner paiameters) was carried out by fitting special forms of the functions [Eqs. (75) and (77)], as described above, and using not more than 10 electronic energies for each of the X H component states, computed at cis- and toans-planai geometries. This procedure led to the above mentioned six parameters... [Pg.527]

You need to specify two parameters the et uilibrium value ofthe internal coordinate and the force constant for the harmonic poten tial, T h e equilibrium restraint value deperi ds on the reason you choosea restraint. If, for example, you would like a particular bond length to remain constant during a simulation, then the equ ilibritirn restrain t value would probably be Lh e initial len gth of the bond. If you wan t to force an internal coordinate to a new value, the equilibrium internal coordinate is the new value. [Pg.105]

The forces between bonded atoms are very strong and considerable energy is required to cause a bond to deviate significantly from its equilibrium value. This is reflected in the magnitude of the force constants for bond stretching some typical values from the MM2 force field are shown in Table 4.1, where it can be seen that those bonds one would... [Pg.189]

We envision a potential energy surface with minima near the equilibrium positions of the atoms comprising the molecule. The MM model is intended to mimic the many-dimensional potential energy surface of real polyatomic molecules. (MM is little used for very small molecules like diatomies.) Once the potential energy surface iias been established for an MM model by specifying the force constants for all forces operative within the molecule, the calculation can proceed. [Pg.98]

There is no force constant for Panslation because it encounters no opposing force. [Pg.286]

When the same energy terms are used in two force helds, it may be acceptable to transfer bond-stretching and angle-bending terms. These are fairly stiff motions that do not change excessively. The force constants for these terms vary between force helds, much more than the unstrained lengths and angles. [Pg.239]

Table 6.1 Force constants for some diatomic molecules... Table 6.1 Force constants for some diatomic molecules...
EA Carter, JT Elynes. Solute-dependent solvent force constants for ion pairs and neutral pairs m a polar solvent. J Phys Chem 93 2184-2187, 1989. [Pg.415]

The Raman and infrared spectra for C70 are much more complicated than for Cfio because of the lower symmetry and the large number of Raman-active modes (53) and infrared active modes (31) out of a total of 122 possible vibrational mode frequencies. Nevertheless, well-resolved infrared spectra [88, 103] and Raman spectra have been observed [95, 103, 104]. Using polarization studies and a force constant model calculation [103, 105], an attempt has been made to assign mode symmetries to all the intramolecular modes. Making use of a force constant model based on Ceo and a small perturbation to account for the weakening of the force constants for the belt atoms around the equator, reasonable consistency between the model calculation and the experimentally determined lattice modes [103, 105] has been achieved. [Pg.55]

Optimize the structure of acetyl radical using the 6-31G(d) basis set at the HF, MP2, B3LYP and QCISD levels of theory. We chose to perform an Opt Freq calculation at the Flartree-Fock level in order to produce initial force constants for the later optimizations (retrieved from the checkpoint file via OptsReadFC). Compare the predicted spin polarizations (listed as part of the population analysis output) for the carbon and oxygen atoms for the various methods to one another and to the experimental values of 0.7 for the C2 carbon atom and 0.2 for the oxygen atom. Note that for the MP2 and QCISD calculations you will need to include the keyword Density=Current in the job s route section, which specifies that the population analysis be performed using the electron density computed by the current theoretical method (the default is to use the Hartree-Fock density). [Pg.130]

Here eK, gk are the force constants for the pure solute K, which can be determined from measurements of its second virial coefficient, and q, oq are similar, but as yet unknown, constants characteristic for the / -hydroquinone lattice. [Pg.29]

The force constants obtained for sulphoxides and sulphones are about 7 x 10 5 and 10 x 10 10 dyne cm - respectively174. The values of the force constants for sulphoxides are very similar to those of the N—O bond in pyridine N-oxides in which the k values are approximately 6-7 x 105 dyne cm-119. [Pg.543]

Rough quantitative calculations of the energy of interaction of the electron pairs and the phonon can be made with use of the force constants for the bonds19 and the changes in the position of the minimum in the potential functions for a bond, as given by the foregoing values of the change in effective radius. [Pg.827]

Kaplan and Thornton (1967) used three different sets of vibrational frequencies to estimate the zero-point energies of the reactants and products of the equilibrium, which provided three different isotope exchange equilibrium constants 1-163, 1-311 and 1-050. The value 1-311 is considered to be most reasonable, whereas the others are rejected as unrealistic for the case in hand. Calculations using the complete theory led to values that varied from 1-086 to 1-774 for different sets of valence-force constants for the compounds involved. [Pg.20]

Changes in observed CH (CD) stretching frequencies on going from reactant to product are found to be too small and in the wrong direction to account for the observed kinetic isotope effect, and the effect is suggested to be due to increased force constants for lower frequency vibrations, such as for bending (Kaplan and Thornton, 1967). This is consistent with a steric explanation. [Pg.20]

The amonotonic order for Co and Ni, compared to the monotonic order for Cu, may best be rationalized in terms of a finite, positive kc=c,c=c interaction force constant for Co and Ni, rather than as the outcome of amonotonicity in the principal c=c force-constants. [Pg.128]

According to Eq. (11), the force constant for the normal vibration Q, can be identified with the term in braces and can be negative if the second term, which is positive, exceeds the first term. If the force constant is negative, the energy should be lowered by the nuclear deformation Qi, and the second-order distortion from the symmetrical nuclear arrangement would occur spontaneously. [Pg.9]


See other pages where Force constants for is mentioned: [Pg.59]    [Pg.2442]    [Pg.480]    [Pg.492]    [Pg.183]    [Pg.194]    [Pg.223]    [Pg.251]    [Pg.505]    [Pg.183]    [Pg.194]    [Pg.204]    [Pg.362]    [Pg.183]    [Pg.445]    [Pg.113]    [Pg.61]    [Pg.231]    [Pg.8]    [Pg.32]    [Pg.33]    [Pg.404]    [Pg.6]    [Pg.15]    [Pg.44]    [Pg.16]    [Pg.43]    [Pg.116]    [Pg.10]    [Pg.12]    [Pg.22]    [Pg.22]   
See also in sourсe #XX -- [ Pg.616 ]

See also in sourсe #XX -- [ Pg.2 , Pg.215 , Pg.216 , Pg.217 , Pg.218 , Pg.232 , Pg.233 , Pg.235 ]




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Force Constants for Bond Stretching

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