Copper(II) complexes based on a new chelating 4-(3,5-diphenyl-1H-pyrazol-1-yl)-6-(piperidin-1-yl)pyrimidine ligand: Synthesis and crystal structures. Lone pair–π, C–H···π, π–π and C–H···A (A=N, Cl) non-covalent interactions

2010 ◽  
Vol 363 (7) ◽  
pp. 1547-1555 ◽  
Author(s):  
Mark B. Bushuev ◽  
Viktor P. Krivopalov ◽  
Natalia V. Pervukhina ◽  
Dmitrii Yu. Naumov ◽  
Gennadii G. Moskalenko ◽  
...  
2020 ◽  
Vol 76 (8) ◽  
pp. 1311-1315
Author(s):  
Andrew Hulsman ◽  
Isabel Lorenzana ◽  
Theodore Schultz ◽  
Breezy Squires ◽  
Brock A. Stenfors ◽  
...  

The syntheses and crystal structures of the two title compounds, C11H10O3 (I) and C17H14BrNO2 (II), both containing the bicyclo[2.2.2]octene ring system, are reported here [the structure of I has been reported previously: White & Goh (2014). Private Communication (refcode HOKRIK). CCDC, Cambridge, England]. The bond lengths and angles of the bicyclo[2.2.2]octene ring system are similar for both structures. The imide functional group of II features carbonyl C=O bond lengths of 1.209 (2) and 1.210 (2) Å, with C—N bond lengths of 1.393 (2) and 1.397 (2) Å. The five-membered imide ring is nearly planar, and it is positioned exo relative to the alkene bridgehead carbon atoms of the bicyclo[2.2.2]octene ring system. Non-covalent interactions present in the crystal structure of II include a number of C—H...O interactions. The extended structure of II also features C—H...O hydrogen bonds as well as C—H...π and lone pair–π interactions, which combine together to create supramolecular sheets.


CrystEngComm ◽  
2018 ◽  
Vol 20 (28) ◽  
pp. 3987-3993 ◽  
Author(s):  
Jorge Echeverría

Ligand⋯ligand contacts, including a novel n → π* interaction involving an isocyanide group as the acceptor, determine the persistent antiparallel conformation of dimers of (isocyanide)Au(i) complexes in their crystal structures.


Molecules ◽  
2018 ◽  
Vol 23 (3) ◽  
pp. 572 ◽  
Author(s):  
Matteo Savastano ◽  
Carla Bazzicalupi ◽  
Palma Mariani ◽  
Antonio Bianchi

2016 ◽  
Vol 72 (12) ◽  
pp. 1762-1767
Author(s):  
Angélica Navarrete Guitérrez ◽  
Gerardo Aguirre Hernández ◽  
Sylvain Bernès

The crystal structures of four bromoarenes based on 2,6-dimethylbromobenzene are reported, which are differentiated according the functional groupXplacedparato the Br atom:X= CN (4-bromo-3,5-dimethylbenzonitrile, C9H8BrN), (1),X= NO2(2-bromo-1,3-dimethyl-5-nitrobenzene, C8H8BrNO2), (2),X= NH2(4-bromo-3,5-dimethylaniline, C8H10BrN), (3) andX= OH (4-bromo-3,5-dimethylphenol, C8H9BrO), (4). The content of the asymmetric unit is different in each crystal,Z′ = ½ (X= CN),Z′ = 1 (X= NO2),Z′ = 2 (X= NH2), andZ′ = 4 (X= OH), and is related to the molecular symmetry and the propensity ofXto be involved in hydrogen bonding. In none of the studied compounds does the crystal structure feature other non-covalent interactions, such as π–π, C—H...π or C—Br...Br contacts.


CrystEngComm ◽  
2020 ◽  
Vol 22 (1) ◽  
pp. 95-104
Author(s):  
Nicole Parra-Muñoz ◽  
Paulina I. Hidalgo ◽  
Gerardo Ripoll ◽  
Julio Belmar ◽  
Jorge Pasán ◽  
...  

Crystal structures of seven new Ag(i) complexes with bis(1-isoquinolinecarboxamide)alkane derivatives were analyzed in terms of the coordinative ability and participation in non-covalent interactions of several counterions.


2011 ◽  
Vol 9 (1) ◽  
pp. 94-105 ◽  
Author(s):  
Rafal Kruszynski ◽  
Tomasz Sieranski

AbstractThe intermolecular non-covalent interactions in aminonitromethylbenzenes namely 2-methyl-4-nitroaniline, 4-methyl-3-nitroaniline, 2-methyl-6-nitroaniline, 4-amino-2,6-dinitrotoluene, 2-methyl-5-nitroaniline, 4-methyl-2-nitroaniline, 2,3-dimethyl-6-nitroaniline, 4,5-dimethyl-2-nitroaniline and 2-methyl-3,5-dinitroaniline were studied by quantum mechanical calculations at RHF/311++G(3df,2p) and B3LYP/311++G(3df,2p) level of theory. The calculations prove that solely geometrical study of hydrogen bonding can be very misleading because not all short distances (classified as hydrogen bonds on the basis of interaction geometry) are bonding in character. For studied compounds interaction energy ranges from 0.23 kcal mol−1 to 5.59 kcal mol−1. The creation of intermolecular hydrogen bonds leads to charge redistribution in donors and acceptors. The Natural Bonding Orbitals analysis shows that hydrogen bonds are created by transfer of electron density from the lone pair orbitals of the H-bond acceptor to the antibonding molecular orbitals of the H-bond donor and Rydberg orbitals of the hydrogen atom. The stacking interactions are the interactions of delocalized molecular π-orbitals of the one molecule with delocalized antibonding molecular π-orbitals and the antibonding molecular σ-orbital created between the carbon atoms of the second aromatic ring and vice versa.


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