Title of article :
Crystal structure, Hirshfeld surface analysis and inter­action energy and DFT studies of 5,5-di­phenyl-1,3-bis­­(prop-2-yn-1-yl)imidazolidine-2,4-dione
Author/Authors :
Ghandour, Ismail Laboratoire de Chimie de la Matière Condensée - Université Sidi Mohamed Ben Abdallah - Faculté des Sciences et Techniques, Morocco , Bouayad, Abdelouahed Laboratoire de Chimie de la Matière Condensée - Université Sidi Mohamed Ben Abdallah - Faculté des Sciences et Techniques, Morocco , Hökelek, Tuncer Department of Physics - Hacettepe University, Turkey , Haoudi, Amal Laboratoire de Chimie Organique Appliquée - Université Sidi Mohamed Ben Abdallah - Faculté des Sciences et Techniques, Morocco , Capet, Frédéric Unité de Catalyse et de Chimie du Solide (UCCS), UMR 8181 - Ecole Nationale Supérieure de Chimie de Lille - Université Lille 1, France , Bouayad, Abdelouahed Unité de Catalyse et de Chimie du Solide (UCCS), UMR 8181 - Ecole Nationale Supérieure de Chimie de Lille - Université Lille 1, France , Kandri Rodi , Youssef Laboratoire de Chimie Organique Appliquée - Université Sidi Mohamed Ben Abdallah - Faculté des Sciences et Techniques, Morocco
Pages :
12
From page :
1
To page :
12
Abstract :
The title compound, C21H16N2O2, consists of an imidazolidine unit linked to two phenyl rings and two prop-2-yn-1-yl moieties. The imidazolidine ring is oriented at dihedral angles of 79.10 (5) and 82.61 (5)° with respect to the phenyl rings, while the dihedral angle between the two phenyl rings is 62.06 (5)°. In the crystal, inter­molecular C—HProp⋯OImdzln (Prop = prop-2-yn-1-yl and Imdzln = imidazolidine) hydrogen bonds link the mol­ecules into infinite chains along the b-axis direction. Two weak C—HPhen⋯π inter­actions are also observed. The Hirshfeld surface analysis of the crystal structure indicates that the most important contributions for the crystal packing are from H⋯H (43.3%), H⋯C/C⋯H (37.8%) and H⋯O/O⋯H (18.0%) inter­actions. Hydrogen bonding and van der Waals inter­actions are the dominant inter­actions in the crystal packing. Computational chemistry indicates that the C—HProp⋯OImdzln hydrogen-bond energy in the crystal is −40.7 kJ mol−1. Density functional theory (DFT) optimized structures at the B3LYP/6–311G(d,p) level are compared with the experimentally determined mol­ecular structure in the solid state. The HOMO–LUMO behaviour was elucidated to determine the energy gap.
Keywords :
crystal structure , oxazole , π-stacking , Hirshfeld surface
Journal title :
Acta Crystallographica Section E: Crystallographic Communications
Serial Year :
2019
Full Text URL :
Record number :
2627657
Link To Document :
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