Carbonyl-Carbonyl Interactions can be Competitive with Hydrogen Bonds
The geometries and attractive energies of carbonyl–carbonyl interactions have been investigated using crystallographic data and ab initio molecular-orbital calculations. Analysis of crystallographic data for 9049 carbon-substituted >C=O groups shows that 1328 (15%) form contacts with other >C=...
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Veröffentlicht in: | Acta crystallographica. Section B, Structural science Structural science, 1998-06, Vol.54 (3), p.320-329 |
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description | The geometries and attractive energies of carbonyl–carbonyl interactions have been investigated using crystallographic data and ab initio molecular-orbital calculations. Analysis of crystallographic data for 9049 carbon-substituted >C=O groups shows that 1328 (15%) form contacts with other >C=O groups, in which d (C...O) < 3.6 Å. Three common interaction motifs are observed in crystal structures: ( a ) a slightly sheared antiparallel motif (650 instances) involving a pair of short C...O interactions, together with ( b ) a perpendicular motif (116 instances) and ( c ) a highly sheared parallel motif (130 instances), which both involve a single short C...O interaction. Together, these motifs account for 945 (71%) of the observed interactions. Ab-initio -based molecular-orbital calculations (6-31G** basis sets), using intermolecular perturbation theory (IMPT) applied to a bis-propanone dimer model, yield an attractive interaction energy of −22.3 kJ mol −1 for a perfect rectangular antiparallel dimer having both d (C...O) = 3.02 Å and attractive energies < −20 kJ mol −1 over the d (C...O) range 2.92–3.32 Å. These energies are comparable to those of medium-strength hydrogen bonds. The IMPT calculations indicate a slight shearing of the antiparallel motif with increasing d (C...O). For the perpendicular motif, IMPT yields an attractive interaction energy of −7.6 kJ mol −1 , comparable in strength to a C—H...O hydrogen bond and with the single d (C...O) again at 3.02 Å. |
doi_str_mv | 10.1107/S0108768198001463 |
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H. ; Baalham, C. A. ; Lommerse, J. P. M. ; Raithby, P. R.</creator><creatorcontrib>Allen, F. H. ; Baalham, C. A. ; Lommerse, J. P. M. ; Raithby, P. R.</creatorcontrib><description>The geometries and attractive energies of carbonyl–carbonyl interactions have been investigated using crystallographic data and ab initio molecular-orbital calculations. Analysis of crystallographic data for 9049 carbon-substituted >C=O groups shows that 1328 (15%) form contacts with other >C=O groups, in which d (C...O) < 3.6 Å. Three common interaction motifs are observed in crystal structures: ( a ) a slightly sheared antiparallel motif (650 instances) involving a pair of short C...O interactions, together with ( b ) a perpendicular motif (116 instances) and ( c ) a highly sheared parallel motif (130 instances), which both involve a single short C...O interaction. Together, these motifs account for 945 (71%) of the observed interactions. Ab-initio -based molecular-orbital calculations (6-31G** basis sets), using intermolecular perturbation theory (IMPT) applied to a bis-propanone dimer model, yield an attractive interaction energy of −22.3 kJ mol −1 for a perfect rectangular antiparallel dimer having both d (C...O) = 3.02 Å and attractive energies < −20 kJ mol −1 over the d (C...O) range 2.92–3.32 Å. These energies are comparable to those of medium-strength hydrogen bonds. The IMPT calculations indicate a slight shearing of the antiparallel motif with increasing d (C...O). For the perpendicular motif, IMPT yields an attractive interaction energy of −7.6 kJ mol −1 , comparable in strength to a C—H...O hydrogen bond and with the single d (C...O) again at 3.02 Å.</description><identifier>ISSN: 0108-7681</identifier><identifier>EISSN: 1600-5740</identifier><identifier>DOI: 10.1107/S0108768198001463</identifier><identifier>CODEN: ASBSDK</identifier><language>eng</language><publisher>5 Abbey Square, Chester, Cheshire CH1 2HU, England: International Union of Crystallography</publisher><subject>Condensed matter: structure, mechanical and thermal properties ; Crystal binding; cohesive energy ; Crystalline state (including molecular motions in solids) ; Exact sciences and technology ; Physics ; Structure of solids and liquids; crystallography</subject><ispartof>Acta crystallographica. 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H.</creatorcontrib><creatorcontrib>Baalham, C. A.</creatorcontrib><creatorcontrib>Lommerse, J. P. M.</creatorcontrib><creatorcontrib>Raithby, P. R.</creatorcontrib><title>Carbonyl-Carbonyl Interactions can be Competitive with Hydrogen Bonds</title><title>Acta crystallographica. Section B, Structural science</title><addtitle>Acta Cryst. B</addtitle><description>The geometries and attractive energies of carbonyl–carbonyl interactions have been investigated using crystallographic data and ab initio molecular-orbital calculations. Analysis of crystallographic data for 9049 carbon-substituted >C=O groups shows that 1328 (15%) form contacts with other >C=O groups, in which d (C...O) < 3.6 Å. Three common interaction motifs are observed in crystal structures: ( a ) a slightly sheared antiparallel motif (650 instances) involving a pair of short C...O interactions, together with ( b ) a perpendicular motif (116 instances) and ( c ) a highly sheared parallel motif (130 instances), which both involve a single short C...O interaction. Together, these motifs account for 945 (71%) of the observed interactions. Ab-initio -based molecular-orbital calculations (6-31G** basis sets), using intermolecular perturbation theory (IMPT) applied to a bis-propanone dimer model, yield an attractive interaction energy of −22.3 kJ mol −1 for a perfect rectangular antiparallel dimer having both d (C...O) = 3.02 Å and attractive energies < −20 kJ mol −1 over the d (C...O) range 2.92–3.32 Å. These energies are comparable to those of medium-strength hydrogen bonds. The IMPT calculations indicate a slight shearing of the antiparallel motif with increasing d (C...O). For the perpendicular motif, IMPT yields an attractive interaction energy of −7.6 kJ mol −1 , comparable in strength to a C—H...O hydrogen bond and with the single d (C...O) again at 3.02 Å.</description><subject>Condensed matter: structure, mechanical and thermal properties</subject><subject>Crystal binding; cohesive energy</subject><subject>Crystalline state (including molecular motions in solids)</subject><subject>Exact sciences and technology</subject><subject>Physics</subject><subject>Structure of solids and liquids; crystallography</subject><issn>0108-7681</issn><issn>1600-5740</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1998</creationdate><recordtype>article</recordtype><recordid>eNqFkLFOwzAURS0EEqXwAWwZWAPPcezYYxtKW1TKAAgxWa5jgyFNKjui5O9JFejCwPSedO65w0XoHMMlxpBdPQAGnjGOBQfAKSMHaIAZQEyzFA7RYIfjHT9GJyG8A0CKOQzQJFd-VVdtGf8-0bxqjFe6cXUVIq2qaGWivF5vTOMa92mirWveollb-PrVVNG4ropwio6sKoM5-7lD9HQzecxn8eJ-Os9Hi1gTKrIYCwF4ZWkiiBaapSSlljFQWBSKcapMkmkOVuPCcFAFT5lKLVXadjhRhpIhwn2v9nUI3li58W6tfCsxyN0O8s8OnXPROxsVtCqtV5V2YS8miWCcQBfjfWzrStP-3ytHL-PZCDDLOjXuVRca87VXlf-QHc2ofF5OZXJH-PWCLuUt-QaN0HvC</recordid><startdate>199806</startdate><enddate>199806</enddate><creator>Allen, F. 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R.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c3597-19901bf5293c9c64345f660a19da685ae27c80fc1de80ad846a4f5acfda62ae53</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1998</creationdate><topic>Condensed matter: structure, mechanical and thermal properties</topic><topic>Crystal binding; cohesive energy</topic><topic>Crystalline state (including molecular motions in solids)</topic><topic>Exact sciences and technology</topic><topic>Physics</topic><topic>Structure of solids and liquids; crystallography</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Allen, F. H.</creatorcontrib><creatorcontrib>Baalham, C. A.</creatorcontrib><creatorcontrib>Lommerse, J. P. M.</creatorcontrib><creatorcontrib>Raithby, P. R.</creatorcontrib><collection>Istex</collection><collection>Pascal-Francis</collection><collection>CrossRef</collection><jtitle>Acta crystallographica. Section B, Structural science</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Allen, F. H.</au><au>Baalham, C. A.</au><au>Lommerse, J. P. M.</au><au>Raithby, P. R.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Carbonyl-Carbonyl Interactions can be Competitive with Hydrogen Bonds</atitle><jtitle>Acta crystallographica. Section B, Structural science</jtitle><addtitle>Acta Cryst. B</addtitle><date>1998-06</date><risdate>1998</risdate><volume>54</volume><issue>3</issue><spage>320</spage><epage>329</epage><pages>320-329</pages><issn>0108-7681</issn><eissn>1600-5740</eissn><coden>ASBSDK</coden><abstract>The geometries and attractive energies of carbonyl–carbonyl interactions have been investigated using crystallographic data and ab initio molecular-orbital calculations. Analysis of crystallographic data for 9049 carbon-substituted >C=O groups shows that 1328 (15%) form contacts with other >C=O groups, in which d (C...O) < 3.6 Å. Three common interaction motifs are observed in crystal structures: ( a ) a slightly sheared antiparallel motif (650 instances) involving a pair of short C...O interactions, together with ( b ) a perpendicular motif (116 instances) and ( c ) a highly sheared parallel motif (130 instances), which both involve a single short C...O interaction. Together, these motifs account for 945 (71%) of the observed interactions. Ab-initio -based molecular-orbital calculations (6-31G** basis sets), using intermolecular perturbation theory (IMPT) applied to a bis-propanone dimer model, yield an attractive interaction energy of −22.3 kJ mol −1 for a perfect rectangular antiparallel dimer having both d (C...O) = 3.02 Å and attractive energies < −20 kJ mol −1 over the d (C...O) range 2.92–3.32 Å. These energies are comparable to those of medium-strength hydrogen bonds. The IMPT calculations indicate a slight shearing of the antiparallel motif with increasing d (C...O). For the perpendicular motif, IMPT yields an attractive interaction energy of −7.6 kJ mol −1 , comparable in strength to a C—H...O hydrogen bond and with the single d (C...O) again at 3.02 Å.</abstract><cop>5 Abbey Square, Chester, Cheshire CH1 2HU, England</cop><pub>International Union of Crystallography</pub><doi>10.1107/S0108768198001463</doi><tpages>10</tpages></addata></record> |
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source | Crystallography Journals Online; Wiley Online Library Journals Frontfile Complete |
subjects | Condensed matter: structure, mechanical and thermal properties Crystal binding cohesive energy Crystalline state (including molecular motions in solids) Exact sciences and technology Physics Structure of solids and liquids crystallography |
title | Carbonyl-Carbonyl Interactions can be Competitive with Hydrogen Bonds |
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