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Internuclear distance, energy and

The aim of this work is to obtain the four lowest E curves and wavefunctions of BH at the same level of accuracy and to bring out the interplay of ionic, Rydberg and valence states at energies and internuclear distances which were not previously investigated. We have therefore made use of a method, already put forward by us [16,17] to determine at once quasi-diabatic and adiabatic states, potential energy cnrves and approximate nonadiabatic couplings. We have analogously determined the first three E+ states, of which only the lowest had been theoretically studied... [Pg.349]

Lippincott, E. R., and R. Schroeder General Relation between Potential Energy and Internuclear Distance. II. Polyatomic Molecules. J. Amer. chem. Soc. 78, 5171-5178 (1956). [Pg.51]

It must be realised that, in view of the assumptions made, these calculations are only approximate, but nevertheless this treatment of the H2+ molecule makes an understanding of the nature of the chemical bond possible. A more exact solution would lead to more complex functions in view of the fact that the electron cloud is really continuous and the division of the cloud into three parts is a considerable simplication. The more exact solutions of Hylleraas and Jaff 2 show almost exact agreement with experiment for values of the bond energy and internuclear distance. [Pg.55]

Table 3.6 LiH dissociation energies and internuclear distances (aug-cc-pVQZ basis set)... Table 3.6 LiH dissociation energies and internuclear distances (aug-cc-pVQZ basis set)...
A parallel exists between electronic energy change and total energy change if we are careful about reference energies and internuclear distances. [Pg.488]

The fact that the nuclei do not get closer together does not mean that the forces of attraction and repulsion are equal. The minimum distance is that distance where the total energy (attraction and repulsion) is most favorable. Because the molecule has some vibrational energy, the internuclear distance is not constant, but the equilibrium distance is Ra. Figure 3.2 shows how the energy of interaction between two hydrogen atoms varies with internuclear distance. [Pg.66]

Electronic Energies, Rotational Constants, and Internuclear Distances of Linear Triatomic Nonhydride Radicals... [Pg.14]

Fig. 12. Calculated binding energy versus internuclear distance for Moj using and C , symmetry constraints and the (a) Xa (Ref. 12) and (b) JMW (Ref. 29) exchange-correlation potentials. (Reproduced from Ref. Fig. 12. Calculated binding energy versus internuclear distance for Moj using and C , symmetry constraints and the (a) Xa (Ref. 12) and (b) JMW (Ref. 29) exchange-correlation potentials. (Reproduced from Ref.
Table XVI. Bond Energy (E) and internuclear distance (R) for hydrogen molecule... Table XVI. Bond Energy (E) and internuclear distance (R) for hydrogen molecule...
The energies of molecular rotational levels, and hence energy differences, depend on the masses that are rotating the heavy nuclei and their geometrical arrangement in space, i.e. the molecular moments of inertia Ix, ly, and (or Ig, lb, and Ic, depending on the coordinate system). For a diatomic molecule of nuclear mass mi and m2, and internuclear distance r, the moment of inertia I is ... [Pg.114]

Figure 4. Variation of H2 total, kinetic, and potential energies with internuclear distance R, as calculated from subhamiltonians (dashed curves) and exact eigenvalues (solid curves). Figure 4. Variation of H2 total, kinetic, and potential energies with internuclear distance R, as calculated from subhamiltonians (dashed curves) and exact eigenvalues (solid curves).
The simplest model of a covalent bond is based on an electrostatic point-charge simulation of overlapping spherical valence-electron charge clouds that surround monopositive atomic cores. For a homonuclear pair of atoms with radius r and internuclear distance d, the dissociation energy D is calculated from... [Pg.94]

The Hamiltonian as well as all following formulas are given in atomic units. The subscripts c and V denote core and valence, respectively, and the Hamiltonian is given for a molecule with valence electrons and N cores with effective core charges Q. ry and denote interelectronic and internuclear distances, respectively. The individual terms of equation 6.1 are the kinetic energy of the valence electrons, the Coulomb interaction between the valence electrons, the superposition of N atomic ECPs point charge Coulomb repulsion... [Pg.149]

The Lennard-Jones 12-6 potential contains just two adjustable parameters the collision diameter a (the separation for which the energy is zero) and the well depth s. These parameters are graphically illustrated in Figure 4.34. The Lennard-Jones equation may also be expressed in terms of the separation at which the energy passes through a minimum, (also written f ). At this separation, the first derivative of the energy with respect to the internuclear distance is zero (i.e. dvjdr = 0), from which it can easily be shown that v = 2 / cr. We can thus also write the Lennard-Jones 12-6 potential function as follows ... [Pg.225]

The calculation of the derivatives T p and Vp means usually a great deal of additional computations, and it is therefore important to observe that, if we are interested only in determining the energy E0 and the internuclear distance R0 for the equilibrium situation, we can use the simpler relations, Eq. 11.25 and Eq. 11.27. In such a case, E0 is the minimum of the quantity... [Pg.223]

In the Extended Hartree-Foek (EHF) technique, the minimization is performed on the form of the PHF wave function. This type of wave function should produce for each interatomic distance a further lowering of the energy with respect to the RHF, UHF, and PHF total energies. The values of E(PHF-FSGO), and E(EHF-FSGO) for internuclear distances from 1.0 a.u. to 7 a.u. (step 0.5 a.u.) are also given in Table 2. As in the UHF... [Pg.195]

We carried out a second calculation for BeH at an internuclear distance of 2.67 a.u. corresponding to the minimum of energy.The mean magnetic susceptibility x obtained value, which is equal to -0,86.lO erg.G. mol V, agrees more closely to the value calculated by Fowler and Steiner [5], at the same internuclear distance,which is equal to -0.50 10 erg. G. mol F... [Pg.315]

The optimization of the geometry leads to a good agreement with experiment for AIH (Rcxp = 1.648 A [25] ). ForMgH a previously calculated internuclear distance [25) using a 6-31G basis set, is equal to 1.863 A which is not very close to our value for this molecule. Note, however, that in the particular case of MgH, the energy presents a flat minimum between 1.79 A and 1.82 A, its variation beeing of the order of lO a.u in this interval. [Pg.315]


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See also in sourсe #XX -- [ Pg.5 , Pg.5 ]




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Internuclear

Internuclear distance

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