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Pauling bond strength, bond length and electron density distribution

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Abstract

The power law regression equation, <R(M–O)> = 1.46(<ρ(r c)>/r)−0.19, relating the average experimental bond lengths, <R(M–O)>, to the average accumulation of the electron density at the bond critical point, <ρ(r c)>, between bonded pairs of metal and oxygen atoms (r is the row number of the M atom), determined at ambient conditions for oxide crystals, is similar to the regression equation R(M–O) = 1.41(ρ(r c)/r)−0.21 determined for three perovskite crystals at pressures as high as 80 GPa. The pair are also comparable with the equation <R(M–O)> = 1.43(<s>/r)−0.21 determined for oxide crystals at ambient conditions and <R(M–O)> = 1.39(<s>/r)−0.22 determined for geometry-optimized hydroxyacid molecules that relate the geometry-optimized bond lengths to the average Pauling bond strength, <s>, for the M–O bonded interactions. On the basis of the correspondence between the equations relating <ρ(r c)> and <s> with bond length, it seems plausible that the Pauling bond strength might serve a rough estimate of the accumulation of the electron density between M–O bonded pairs of atoms. Similar expressions, relating bond length and bond strength hold for fluoride, nitride and sulfide molecules and crystals. The similarity of the expressions for the crystals and molecules is compelling evidence that molecular and crystalline M–O bonded interactions are intrinsically related. The value of <ρ(r c)> = r[(1.41)/<R(M–O)>]4.76 determined for the average bond length for a given coordination polyhedron closely matches the Pauling’s electrostatic bond strength reaching each the coordinating anions of the coordinated polyhedron. Despite the relative simplicity of the expression, it appears to be more general in its application in that it holds for the bulk of the M–O bonded pairs of atoms of the periodic table.

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Acknowledgments

The work was supported in part by the National Science Foundation and the U.S. Department of Energy through grants to N.L.R. (Grant Nos. EAR-0738692 and EAR-1118691) and D.F.C. (Grant No. DEFG02-97ER14751). K.M.R. acknowledges support from US Department of Energy (DOE), Office of Basic Energy Sciences, Chemical Sciences, Geosciences and Biosciences Division. The bulk of this study was supported by a Virginia Tech University Distinguished Professor Virginia Travel Grant to G.V.G. together with a Jack Phillips Bequeath for generous support during his visit and collaboration with Mark Spackman at the School of Chemistry and Biochemistry, University of Western Australia in Australia and travel support from the Danish National Research Foundation for his visit and to participate in a symposium at the Department of Chemistry, Aarhus University in Denmark and his collaboration with Bo Iversen. G.V.G. also wishes to thank Prof. Vladimir Tsirelson, Head of the Quantum Chemistry Department at the Mendeleev University of Chemical Technology, Miusskaya, Moscow, Russia for bringing to his attention that the electron density distribution between the bonded carbon atoms of diamond is consistent with a power law rather than a exponential law relationship. Finally, we wish to thank the two reviewers of the manuscript who made a number of very important suggestions that definitely improved the manuscript. We are particularly grateful to Frank Hawthorne for suggesting a number of important changes in the text. The paper reads much better because of the reviewer’s efforts and suggestions.

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Gibbs, G.V., Ross, N.L., Cox, D.F. et al. Pauling bond strength, bond length and electron density distribution. Phys Chem Minerals 41, 17–25 (2014). https://doi.org/10.1007/s00269-013-0619-z

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