4.6 Article

Orbital overlap and chemical bonding

Journal

CHEMISTRY-A EUROPEAN JOURNAL
Volume 12, Issue 36, Pages 9196-9216

Publisher

WILEY-V C H VERLAG GMBH
DOI: 10.1002/chem.200600564

Keywords

bond energy; bond theory; density functional calculations; energy decomposition analysis; main group elements

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The chemical bonds in the diatomic molecules Li-2-F-2 and Na-2-Cl-2 at different bond lengths have been analyzed by the energy decomposition analysis (EDA) method using DFT calculations at the BP86/TZ2P level. The interatomic interactions are discussed in terms of quasiclassical electrostatic interactions Delta E-elstat, Pauli repulsion Delta E-Pauli and attractive orbital interactions Delta E-Pauli. The energy terms are compared with the orbital overlaps at different interatomic distances. The quasiclassical electrostatic interactions between two electrons occupying 1s, 2s, 2p(sigma), and 2p(pi) orbitals have been calculated and the results are analyzed and discussed. It is shown that the equilibrium distances of the covalent bonds are not determined by the maximum overlap of the sigma valence orbitals, which nearly always has its largest value at clearly shorter distances than the equilibrium bond length. The crucial interaction that prevents shorter bonds is not the loss of attractive interactions, but a sharp increase in the Pauli repulsion between electrons in valence orbitals. The attractive interactions of Delta E-orb and the repulsive interactions of Delta E-orb are both determined by the orbital overlap. The net effect of the two terms depends on the occupation of the valence orbitals, but the onset of attractive orbital interactions occurs at longer distances than Pauli repulsion, because overlap of occupied orbitals with vacant orbitals starts earlier than overlap between occupied orbitals. The contribution of Delta E-elslat in most nonpolar covalent bonds is strongly attractive. This comes from the deviation of quasiclassical electron-electron repulsion and nuclear-electron attraction from Coulomb's law for point charges. The actual strength of Delta E-elstat depends on the size and shape of the occupied valence orbitals. The attractive electrostatic contributions in the diatomic molecules Li-2-F-2 come from the s and p(sigma) electrons, while the p(pi) electrons do not compensate for nuclear-nuclear repulsion. It is the interplay of the three terms Delta E-orb, Delta E-Pauli, and Delta E-elstat that determines the bond energies and equilibrium distances of covalently bonded molecules. Molecules like N-2 and O-2, which are usually considered as covalently bonded, would not be bonded without the quasiclassical attraction Delta E-elstat.

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