Crystal structure, Hirshfeld surface analysis, interaction energy and DFT studies of 4-[(4-allyl-2- methoxyphenoxy)methyl]-1-(4-methoxyphenyl)- 1H-1,2,3-triazole.

Autor: Taia, Abdelmaoujoud, Essaber, Mohamed, Aatif, Abdeljalil, Chkirate, Karim, Hökelek, Tuncer, Mague, Joel T., Sebbar, Nada Kheira
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Zdroj: Acta Crystallographica Section E: Crystallographic Communications; Jun2020, Vol. 76 Issue 6, p962-966, 11p
Abstrakt: In the title mol­ecule, C20H21N3O3, the allyl substituent is rotated out of the plane of its attached phenyl ring [torsion angle 100.66 (15)°]. In the crystal, C—HMthphn...OMthphn (Mthphn = meth­oxy­phen­yl) hydrogen bonds lead to the formation of (100) layers that are connected into a three-dimensional network by C—H...π(ring) inter­actions, together with π–π stacking inter­actions [centroid-to-centroid distance = 3.7318 (10) Å] between parallel phenyl rings. Hirshfeld surface analysis indicates that the most important contributions to the crystal packing are from H...H (48.7%) and H...C/C...H (23.3%) inter­actions. Computational chemistry reveals that the C—HMthphn...OMthphn hydrogen bond energy is 47.1 kJ mol−1. The theoretical structure, optimized by density functional theory (DFT) at the B3LYP/ 6–311 G(d,p) level, is compared with the experimentally determined mol­ecular structure. The HOMO–LUMO behaviour was elucidated to determine the energy gap. [ABSTRACT FROM AUTHOR]
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