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The multiple bonding in heavier group 14 element alkene analogues is stabilized mainly by dispersion force effects
The structures and bonding in the heavier group 14 element olefin analogues [E{CH(SiMe(3))(2)}(2)](2) and [E{N(SiMe(3))(2)}(2)](2) (E = Ge, Sn, or Pb) and their dissociation into :E{CH(SiMe(3))(2)}(2) and :E{N(SiMe(3))(2)}(2) monomers were studied computationally using hybrid density functional theo...
Autores principales: | , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
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Royal Society of Chemistry
2015
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6054042/ https://www.ncbi.nlm.nih.gov/pubmed/30090241 http://dx.doi.org/10.1039/c5sc02707a |
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author | Guo, Jing-Dong Liptrot, David J. Nagase, Shigeru Power, Philip P. |
author_facet | Guo, Jing-Dong Liptrot, David J. Nagase, Shigeru Power, Philip P. |
author_sort | Guo, Jing-Dong |
collection | PubMed |
description | The structures and bonding in the heavier group 14 element olefin analogues [E{CH(SiMe(3))(2)}(2)](2) and [E{N(SiMe(3))(2)}(2)](2) (E = Ge, Sn, or Pb) and their dissociation into :E{CH(SiMe(3))(2)}(2) and :E{N(SiMe(3))(2)}(2) monomers were studied computationally using hybrid density functional theory (DFT) at the B3PW91 with basis set superposition error and zero point energy corrections. The structures were reoptimized with the dispersion-corrected B3PW91-D3 method to yield dispersion force effects. The calculations generally reproduced the experimental structural data for the tetraalkyls with a few angular exceptions. For the alkyls, without the dispersion corrections, dissociation energies of –2.3 (Ge), +2.1 (Sn), and –0.6 (Pb) kcal mol(–1) were calculated, indicating that the dimeric E–E bonded structure is favored only for tin. However, when dispersion force effects are included, much higher dissociation energies of 28.7 (Ge), 26.3 (Sn), and 15.2 (Pb) kcal mol(–1) were calculated, indicating that all three E–E bonded dimers are favored. Calculated thermodynamic data at 25 °C and 1 atm for the dissociation of the alkyls yield ΔG values of 9.4 (Ge), 7.1 (Sn), and –1.7 (Pb) kcal mol(–1), indicating that the dimers of Ge and Sn, but not Pb, are favored. These results are in harmony with experimental data. The dissociation energies for the putative isoelectronic tetraamido-substituted dimers [E{N(SiMe(3))(2)}(2)](2) without dispersion correction are –7.0 (Ge), –7.4 (Sn), and –4.8 (Pb) kcal mol(–1), showing that the monomers are favored in all cases. Inclusion of the dispersion correction yields the values 3.6 (Ge), 11.7 (Sn), and 11.8 (Pb) kcal mol(–1), showing that dimerization is favored but less strongly so than in the alkyls. The calculated thermodynamic data for the amido germanium, tin, and lead dissociation yield ΔG values of –12.2, –3.7, and –3.6 kcal mol(–1) at 25 °C and 1 atm, consistent with the observation of monomeric structures. Overall, these data indicate that, in these sterically-encumbered molecules, dispersion force attraction between the ligands is of greater importance than group 14 element–element bonding, and is mainly responsible for the dimerization of the metallanediyls species to give the dimetallenes. In addition, calculations on the non-dissociating distannene [Sn{SiMe(t)Bu(2)}(2)](2) show that the attractive dispersion forces are key to its stability. |
format | Online Article Text |
id | pubmed-6054042 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2015 |
publisher | Royal Society of Chemistry |
record_format | MEDLINE/PubMed |
spelling | pubmed-60540422018-08-08 The multiple bonding in heavier group 14 element alkene analogues is stabilized mainly by dispersion force effects Guo, Jing-Dong Liptrot, David J. Nagase, Shigeru Power, Philip P. Chem Sci Chemistry The structures and bonding in the heavier group 14 element olefin analogues [E{CH(SiMe(3))(2)}(2)](2) and [E{N(SiMe(3))(2)}(2)](2) (E = Ge, Sn, or Pb) and their dissociation into :E{CH(SiMe(3))(2)}(2) and :E{N(SiMe(3))(2)}(2) monomers were studied computationally using hybrid density functional theory (DFT) at the B3PW91 with basis set superposition error and zero point energy corrections. The structures were reoptimized with the dispersion-corrected B3PW91-D3 method to yield dispersion force effects. The calculations generally reproduced the experimental structural data for the tetraalkyls with a few angular exceptions. For the alkyls, without the dispersion corrections, dissociation energies of –2.3 (Ge), +2.1 (Sn), and –0.6 (Pb) kcal mol(–1) were calculated, indicating that the dimeric E–E bonded structure is favored only for tin. However, when dispersion force effects are included, much higher dissociation energies of 28.7 (Ge), 26.3 (Sn), and 15.2 (Pb) kcal mol(–1) were calculated, indicating that all three E–E bonded dimers are favored. Calculated thermodynamic data at 25 °C and 1 atm for the dissociation of the alkyls yield ΔG values of 9.4 (Ge), 7.1 (Sn), and –1.7 (Pb) kcal mol(–1), indicating that the dimers of Ge and Sn, but not Pb, are favored. These results are in harmony with experimental data. The dissociation energies for the putative isoelectronic tetraamido-substituted dimers [E{N(SiMe(3))(2)}(2)](2) without dispersion correction are –7.0 (Ge), –7.4 (Sn), and –4.8 (Pb) kcal mol(–1), showing that the monomers are favored in all cases. Inclusion of the dispersion correction yields the values 3.6 (Ge), 11.7 (Sn), and 11.8 (Pb) kcal mol(–1), showing that dimerization is favored but less strongly so than in the alkyls. The calculated thermodynamic data for the amido germanium, tin, and lead dissociation yield ΔG values of –12.2, –3.7, and –3.6 kcal mol(–1) at 25 °C and 1 atm, consistent with the observation of monomeric structures. Overall, these data indicate that, in these sterically-encumbered molecules, dispersion force attraction between the ligands is of greater importance than group 14 element–element bonding, and is mainly responsible for the dimerization of the metallanediyls species to give the dimetallenes. In addition, calculations on the non-dissociating distannene [Sn{SiMe(t)Bu(2)}(2)](2) show that the attractive dispersion forces are key to its stability. Royal Society of Chemistry 2015-11-01 2015-08-19 /pmc/articles/PMC6054042/ /pubmed/30090241 http://dx.doi.org/10.1039/c5sc02707a Text en This journal is © The Royal Society of Chemistry 2015 https://creativecommons.org/licenses/by/3.0/This article is freely available. This article is licensed under a Creative Commons Attribution 3.0 Unported Licence (CC BY 3.0) |
spellingShingle | Chemistry Guo, Jing-Dong Liptrot, David J. Nagase, Shigeru Power, Philip P. The multiple bonding in heavier group 14 element alkene analogues is stabilized mainly by dispersion force effects |
title | The multiple bonding in heavier group 14 element alkene analogues is stabilized mainly by dispersion force effects
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title_full | The multiple bonding in heavier group 14 element alkene analogues is stabilized mainly by dispersion force effects
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title_fullStr | The multiple bonding in heavier group 14 element alkene analogues is stabilized mainly by dispersion force effects
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title_full_unstemmed | The multiple bonding in heavier group 14 element alkene analogues is stabilized mainly by dispersion force effects
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title_short | The multiple bonding in heavier group 14 element alkene analogues is stabilized mainly by dispersion force effects
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title_sort | multiple bonding in heavier group 14 element alkene analogues is stabilized mainly by dispersion force effects |
topic | Chemistry |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6054042/ https://www.ncbi.nlm.nih.gov/pubmed/30090241 http://dx.doi.org/10.1039/c5sc02707a |
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