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N,N′-Bis(pyridin-4-ylmeth­yl)oxalamide benzene monosolvate: crystal structure, Hirshfeld surface analysis and computational study

The asymmetric unit of the title 1:1 solvate, C(14)H(14)N(4)O(2)·C(6)H(6) [systematic name of the oxalamide mol­ecule: N,N′-bis­(pyridin-4-ylmeth­yl)ethanedi­amide], comprises a half mol­ecule of each constituent as each is disposed about a centre of inversion. In the oxalamide mol­ecule, the centra...

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Detalles Bibliográficos
Autores principales: Tan, Sang Loon, Halcovitch, Nathan R., Tiekink, Edward R. T.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: International Union of Crystallography 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6690468/
https://www.ncbi.nlm.nih.gov/pubmed/31417779
http://dx.doi.org/10.1107/S2056989019009551
Descripción
Sumario:The asymmetric unit of the title 1:1 solvate, C(14)H(14)N(4)O(2)·C(6)H(6) [systematic name of the oxalamide mol­ecule: N,N′-bis­(pyridin-4-ylmeth­yl)ethanedi­amide], comprises a half mol­ecule of each constituent as each is disposed about a centre of inversion. In the oxalamide mol­ecule, the central C(2)N(2)O(2) atoms are planar (r.m.s. deviation = 0.0006 Å). An intra­molecular amide-N—H⋯O(amide) hydrogen bond is evident, which gives rise to an S(5) loop. Overall, the mol­ecule adopts an anti­periplanar disposition of the pyridyl rings, and an orthogonal relationship is evident between the central plane and each terminal pyridyl ring [dihedral angle = 86.89 (3)°]. In the crystal, supra­molecular layers parallel to (10[Image: see text]) are generated owing the formation of amide-N—H⋯N(pyrid­yl) hydrogen bonds. The layers stack encompassing benzene mol­ecules which provide the links between layers via methyl­ene-C—H⋯π(benzene) and benzene-C—H⋯π(pyrid­yl) inter­actions. The specified contacts are indicated in an analysis of the calculated Hirshfeld surfaces. The energy of stabilization provided by the conventional hydrogen bonding (approximately 40 kJ mol(−1); electrostatic forces) is just over double that by the C—H⋯π contacts (dispersion forces).