Klopman-Salem equation

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In the theory of chemical reactivity, the Klopman-Salem equation describes the energetic change that occurs when two species approach each other in the course of a reaction and begin to interact, as their associated molecular orbitals begin to overlap with each other and atoms bearing partial charges begin to experience attractive or repulsive electrostatic forces. First described independently by Gilles Klopman [1] and Lionel Salem [2] in 1968, this relationship provides a mathematical basis for the key assumptions of frontier molecular orbital theory (i.e., theory of HOMO-LUMO interactions) and hard soft acid base (HSAB) theory. Conceptually, it highlights the importance of considering both electrostatic interactions and orbital interactions (and weighing the relative significance of each) when rationalizing the selectivity or reactivity of a chemical process.

In chemistry, reactivity is the impetus for which a chemical substance undergoes a chemical reaction, either by itself or with other materials, with an overall release of energy.

A chemical species is a chemical substance or ensemble composed of chemically identical molecular entities that can explore the same set of molecular energy levels on a characteristic or delineated time scale. The term is applied equally to a set of chemically identical atomic or molecular structural units in a solid array.

Molecular orbital energy level in a molecule

In chemistry, a molecular orbital (MO) is a mathematical function describing the wave-like behavior of an electron in a molecule. This function can be used to calculate chemical and physical properties such as the probability of finding an electron in any specific region. The term orbital was introduced by Robert S. Mulliken in 1932 as an abbreviation for one-electron orbital wave function. At an elementary level, it is used to describe the region of space in which the function has a significant amplitude. Molecular orbitals are usually constructed by combining atomic orbitals or hybrid orbitals from each atom of the molecule, or other molecular orbitals from groups of atoms. They can be quantitatively calculated using the Hartree–Fock or self-consistent field (SCF) methods.

Formulation and interpretation

In modern form, [3] the Klopman-Salem equation is commonly given as

,

where

is the electron population in atomic orbital a,

, are the resonance and overlap integrals for the interaction of atomic orbitals a and b,

is the total charge on atom k,

is the local dielectric constant,

is the distance between the nuclei of atoms k and l,

is the coefficient of atomic orbital a in molecular orbital r,

and is the energy of molecular orbital r.

Broadly speaking, the first term describes the closed-shell repulsion of the occupied molecular orbitals of the reactants (four-electron filled-filled interactions, steric effects [4] ). The second term describes the Coulombic attraction or repulsion between the atoms of the reactants (ionic contribution, electrostatic effects). Finally, the third term accounts for all possible interactions between the occupied and unoccupied molecular orbitals of the reactants (two-electron filled-unfilled interactions, stereoelectronic effects [5] ). Although conceptually useful, the Klopman-Salem equation seldom serves as the basis for energetic analysis in modern quantum chemical calculations.

Because of the difference in MO energies appearing in the denominator of the third term, energetically close orbitals make the biggest contribution. Hence, approximately speaking, analysis can often be simplified by considering only the highest occupied and lowest unoccupied molecular orbitals of the reactants (the HOMO-LUMO interaction in frontier molecular orbital theory). [6] The relative contributions of the second (ionic) and third (covalent) terms play an important role in justifying hard soft acid base theory (HSAB), with hard-hard interactions governed by the ionic term and soft-soft interactions governed by the covalent term. [7]

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References

  1. Klopman, Gilles (1968-01-01). "Chemical reactivity and the concept of charge- and frontier-controlled reactions". Journal of the American Chemical Society. 90 (2): 223–234. doi:10.1021/ja01004a002. ISSN   0002-7863.
  2. Salem, Lionel (1968-01-01). "Intermolecular orbital theory of the interaction between conjugated systems. I. General theory". Journal of the American Chemical Society. 90 (3): 543–552. doi:10.1021/ja01005a001. ISSN   0002-7863.
  3. Fleming, Ian (1976). Frontier Orbitals and Organic Chemical Reactions (Reprinted 2006 ed.). Chichester, UK: Wiley. p. 27. ISBN   978-0471018209.
  4. The term steric effects is broad and often includes the result of Coulombic repulsion as well, since, in practice, any method of dividing energetic contributions between repulsive electrostatic interactions and filled-orbital repulsion is artificial and arbitrary to varying degrees.
  5. The term stereoelectronic effects usually refers to the consequence of energetically favorable, two-orbital, two-electron interactions; however, it can be used more broadly to refer to any effect originating from orbital interaction, including unfavorable two-orbital, four-electron interactions.
  6. Fukui, Kenichi (1982). "Role of Frontier Orbitals in Chemical Reactions". Science. 218 (4574): 747–754. Bibcode:1982Sci...218..747F. doi:10.1126/science.218.4574.747. JSTOR   1689733. PMID   17771019.
  7. Pearson, Ralph G. (1997). "The HSAB Principle". Chemical Hardness. Wiley-VCH Verlag GmbH & Co. KGaA. pp. 1–27. doi:10.1002/3527606173.ch1. ISBN   9783527606177.