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The Dihydrogen Molecule

Here the integration J dr is over the coordinates of both electrons. Such integrals are therefore eight-dimensional (three spatial variables and one spin variable per electron). Integration over the spin variables is straightforward, but the spatial variables are far from easy a particular source of trouble arises from the electron repulsion term. [Pg.92]

In the case of the hydrogen molecule-ion H2 , we defined certain integrals Saa, Taa, Tab, Labra- The electronic part of the energy appropriate to the Heitler-London (singlet) ground-state wavefunction, after doing the integrations [Pg.92]

Single hydrogenic Is valence bond Heitler and London f = 1 3.156 86.8 [Pg.94]

We often refer to Heitler and London s method as the valence bond (VB) model. A comparison between the experimental and the valence bond potential energy curves shows excellent agreement at large 7 ab but poor quantitative agreement in the valence region (Table 4.3). The cause of this lies in the method itself the VB model starts from atomic wavefunctions and adds as a perturbation the fact that the electron clouds of the atoms are polarized when the molecule is formed. [Pg.94]

A slight improvement in the predicted dissociation energy occurs if the Is orbital exponent is treated as a variational parameter. [Pg.94]

27 aa + 2Sab ab 2Vaara 2Vaarb 4SabVabra + aabb + abab [Pg.93]


The two preceding applications showed that our hydrogenic model fits well with the helium atom and the dihydrogen molecule for the determination of the polarization functions except that their exponent ( is different from Co which is the exponent of the genuine basis set It is obvious that the hydrogenic model will fit less and... [Pg.276]

The third major mechanism is based on homolytic cleavage of the dihydrogen molecule by metal-metal (Co) bonded species or by a paramagnetic complex (equations 3 and 4)15. [Pg.993]

The dihydrogen molecule assumes a side-on terminal coordination. The W-H2 distance is 1.95 A (X-ray diffraction) or 1.89 A (neutron diffraction). The H-H distance is 0.75 A (X-ray diffraction) or 0.82 A (neutron diffraction), with respect to 0.74 A for molecular hydrogen in the gaseous state. [Pg.486]

Woelk and coworkers [252, 270] have provided a detailed view into the activation and transfer of the dihydrogen molecule during hydrogenations in SCCO2, using PHIP and their toroid cavity NMR autoclave. For the asymmetric hydrogenation... [Pg.63]

The dihydrogen molecule is the smallest molecule in existence. It has a strong covalent bond with a dissociation energy of 103 kcal mol [1], In a hydrogenation reaction, this bond has to be broken and two new C-H bonds are formed, one of the simplest forms of chemical reaction. [Pg.360]

This process does not necessarily have to be simultaneous, but the two atoms of the dihydrogen molecule must retain a spin-spin coupling throughout the whole process. Conversely, if they are not transferred pair-wise (i. e., if the transferred hydrogen atoms stem from different dihydrogen molecules or if they lose their coupling in the course of the process), no polarization can be detected. [Pg.367]

Covalent Bonding I the Dihydrogen Molecule-ion, H2+, and the Dihydrogen Molecule... [Pg.34]

This chapter consists of the application of the symmetry concepts of Chapter 2 to the construction of molecular orbitals for a range of diatomic molecules. The principles of molecular orbital theory are developed in the discussion of the bonding of the simplest molecular species, the one-electron dihydrogen molecule-ion, H2+, and the simplest molecule, the two-electron dihydrogen molecule. Valence bond theory is introduced and compared with molecular orbital theory. The photo-electron spectrum of the dihydrogen molecule is described and interpreted. [Pg.34]

The application of group theory to define the orbitals of the dihydrogen molecule... [Pg.34]

The molecular orbital theory of the dihydrogen molecule is dealt with in detail above, and describes how the two electrons occupy a bonding molecular orbital so that they are equally shared between the two nuclei. This state of affairs can be written symbolically in the form ... [Pg.48]

To obtain an accurate assessment of the interelectronic repulsion energy of the H2 molecule it is essential to carry out calculations in which the hydrogen nuclei are a constant distance apart. The following calculations are for an internuclear distance of 74 pm for both molecules, which is the equilibrium internuclear distance in the dihydrogen molecule. [Pg.50]


See other pages where The Dihydrogen Molecule is mentioned: [Pg.92]    [Pg.428]    [Pg.342]    [Pg.378]    [Pg.257]    [Pg.98]    [Pg.72]    [Pg.95]    [Pg.359]    [Pg.360]    [Pg.363]    [Pg.363]    [Pg.366]    [Pg.376]    [Pg.226]    [Pg.21]    [Pg.34]    [Pg.34]    [Pg.37]    [Pg.41]    [Pg.46]    [Pg.49]    [Pg.51]    [Pg.51]    [Pg.52]   


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Dihydrogen molecule

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