Synthesis of two new Schiff bases; crystal structure, Hirshfeld surface analysis, density functional theory and molecular docking

2021 ◽  
Vol 1226 ◽  
pp. 129330
Author(s):  
Muhammad Asam Raza ◽  
Necmi DEGE ◽  
Onur Erman DOĞAN ◽  
Tuğgan AĞAR ◽  
Sajjad Hussain Sumrra
Author(s):  
Ballo Daouda ◽  
Nanou Tiéba Tuo ◽  
Tuncer Hökelek ◽  
Kangah Niameke Jean-Baptiste ◽  
Kodjo Charles Guillaume ◽  
...  

The title compound, C18H16N2O2, consists of perimidine and methoxyphenol units, where the tricyclic perimidine unit contains a naphthalene ring system and a non-planar C4N2 ring adopting an envelope conformation with the NCN group hinged by 47.44 (7)° with respect to the best plane of the other five atoms. In the crystal, O—HPhnl...NPrmdn and N—HPrmdn...OPhnl (Phnl = phenol and Prmdn = perimidine) hydrogen bonds link the molecules into infinite chains along the b-axis direction. Weak C—H...π interactions may further stabilize the crystal structure. The Hirshfeld surface analysis of the crystal structure indicates that the most important contributions for the crystal packing are from H...H (49.0%), H...C/C...H (35.8%) and H...O/O...H (12.0%) interactions. Hydrogen bonding and van der Waals interactions are the dominant interactions in the crystal packing. Computational chemistry indicates that in the crystal, the O—HPhnl...NPrmdn and N—HPrmdn...OPhnl hydrogen-bond energies are 58.4 and 38.0 kJ mol−1, respectively. Density functional theory (DFT) optimized structures at the B3LYP/ 6–311 G(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.


Author(s):  
Mohamed Srhir ◽  
Nada Kheira Sebbar ◽  
Tuncer Hökelek ◽  
Ahmed Moussaif ◽  
Joel T. Mague ◽  
...  

In the title molecule, C12H13N3O2S, the benzothiazine moiety is slightly non-planar, with the imidazolidine portion twisted only a few degrees out of the mean plane of the former. In the crystal, a layer structure parallel to the bc plane is formed by a combination of O—HHydethy...NThz hydrogen bonds and weak C—HImdz...OImdz and C—HBnz...OImdz (Hydethy = hydroxyethyl, Thz = thiazole, Imdz = imidazolidine and Bnz = benzene) interactions, together with C—HImdz...π(ring) and head-to-tail slipped π-stacking [centroid-to-centroid distances = 3.6507 (7) and 3.6866 (7) Å] interactions between thiazole rings. The Hirshfeld surface analysis of the crystal structure indicates that the most important contributions for the crystal packing are from H...H (47.0%), H...O/O...H (16.9%), H...C/C...H (8.0%) and H...S/S...H (7.6%) interactions. Hydrogen bonding and van der Waals interactions are the dominant interactions in the crystal packing. Computational chemistry indicates that in the crystal, C—H...N and C—H...O hydrogen-bond energies are 68.5 (for O—HHydethy...NThz), 60.1 (for C—HBnz...OImdz) and 41.8 kJ mol−1 (for C—HImdz...OImdz). Density functional theory (DFT) optimized structures at the B3LYP/6–311 G(d,p) level are compared with the experimentally determined molecular structure in the solid state.


2019 ◽  
Vol 75 (10) ◽  
pp. 1411-1417
Author(s):  
Sonia Hayani ◽  
Yassir Filali Baba ◽  
Tuncer Hökelek ◽  
Fouad Ouazzani Chahdi ◽  
Joel T. Mague ◽  
...  

The title compound, C15H12ClNO3, consists of a 1,2-dihydroquinoline-4-carboxylate unit with 2-chloroethyl and propynyl substituents, where the quinoline moiety is almost planar and the propynyl substituent is nearly perpendicular to its mean plane. In the crystal, the molecules form zigzag stacks along the a-axis direction through slightly offset π-stacking interactions between inversion-related quinoline moieties which are tied together by intermolecular C—HPrpnyl...OCarbx and C—HChlethy...OCarbx (Prpnyl = propynyl, Carbx = carboxylate and Chlethy = chloroethyl) hydrogen bonds. The Hirshfeld surface analysis of the crystal structure indicates that the most important contributions for the crystal packing are from H...H (29.9%), H...O/O...H (21.4%), H...C/C... H (19.4%), H...Cl/Cl...H (16.3%) and C...C (8.6%) interactions. Hydrogen bonding and van der Waals interactions are the dominant interactions in the crystal packing. Computational chemistry indicates that in the crystal, the C—HPrpnyl...OCarbx and C—HChlethy...OCarbx hydrogen bond energies are 67.1 and 61.7 kJ mol−1, respectively. Density functional theory (DFT) optimized structures at the B3LYP/ 6–311 G(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.


2020 ◽  
Vol 76 (7) ◽  
pp. 1075-1079
Author(s):  
Nermin Kahveci Yagci ◽  
Md. Serajul Haque Faizi ◽  
Alev Sema Aydin ◽  
Necmi Dege ◽  
Onur Erman Dogan ◽  
...  

In the title compound, C15H15NO, the configuration of the C=N bond of the Schiff base is E, and an intramolecular O—H...N hydrogen bond is observed, forming an intramolecular S(6) ring motif. The phenol ring is inclined by 45.73 (2)° from the plane of the aniline ring. In the crystal, molecules are linked along the b axis by O—H...N and C—H...O hydrogen bonds, forming polymeric chains. The Hirshfeld surface analysis of the crystal structure indicates that the most important contributions for the packing arrangement are from H...H (56.9%) and H...C/C...H (31.2%) interactions. The density functional theory (DFT) optimized structure at the B3LYP/ 6–311 G(d,p) level is compared with the experimentally determined molecular structure, and the HOMO–LUMO energy gap is provided. The crystal studied was refined as an inversion twin.


Author(s):  
Ahlam Idrissi ◽  
Karim Chkirate ◽  
Nadeem Abad ◽  
Bahia Djerrari ◽  
Redouane Achour ◽  
...  

In the title molecule, C13H13N3O, the isoxazole ring is inclined to the benzimidazole ring at a dihedral angle of 69.28 (14)°. In the crystal, N—H...N hydrogen bonds between neighboring benzimidazole rings form chains along the a-axis direction. Hirshfeld surface analysis indicates that the most important contributions to the crystal packing are from H...H (48.8%), H...C/C...H (20.9%) and H...N/N...H (19.3%) interactions. The optimized structure calculated using density functional theory at the B3LYP/6–311 G(d,p) level is compared with the experimentally determined structure in the solid state. The calculated highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) energy gap is 4.9266 eV.


2019 ◽  
Vol 75 (11) ◽  
pp. 1672-1678
Author(s):  
Mouad Filali ◽  
Lhoussaine El Ghayati ◽  
Tuncer Hökelek ◽  
Joel T. Mague ◽  
Abdessalam Ben-Tama ◽  
...  

The title compound, C22H16N4O2, contains two pyridine rings and one methoxycarbonylphenyl group attached to a pyridazine ring which deviates very slightly from planarity. In the crystal, ribbons consisting of inversion-related chains of molecules extending along the a-axis direction are formed by C—HMthy...OCarbx (Mthy = methyl and Carbx = carboxylate) hydrogen bonds. The ribbons are connected into layers parallel to the bc plane by C—HBnz...π(ring) (Bnz = benzene) interactions. The Hirshfeld surface analysis of the crystal structure indicates that the most important contributions for the crystal packing are from H...H (39.7%), H...C/C...H (27.5%), H...N/N...H (15.5%) and O...H/H...O (11.1%) interactions. Hydrogen-bonding and van der Waals interactions are the dominant interactions in the crystal packing. Computational chemistry indicates that in the crystal, C—HMthy...OCarbx hydrogen-bond energies are 62.0 and 34.3 kJ mol−1, respectively. 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.


Author(s):  
Abdelmaoujoud Taia ◽  
Mohamed Essaber ◽  
Tuncer Hökelek ◽  
Abdeljalil Aatif ◽  
Joel T. Mague ◽  
...  

The asymmetric unit of the title compound, C23H28O4, comprises two half-molecules, with the other half of each molecule being completed by the application of twofold rotation symmetry. The two completed molecules both have a V-shaped appearance but differ in their conformations. In the crystal, each independent molecule forms chains extending parallel to the b axis with its symmetry-related counterparts through C—H...π(ring) interactions. Hirshfeld surface analysis of the crystal structure indicates that the most important contributions for the crystal packing are from H...H (65.4%), H...C/C...H (21.8%) and H...O/O...H (12.3%) interactions. Optimized structures using density functional theory (DFT) at the B3LYP/6–311 G(d,p) level are compared with the experimentally determined molecular structures in the solid state. The HOMO–LUMO behaviour was elucidated to determine the energy gap.


Author(s):  
Nadeem Abad ◽  
Karim Chkirate ◽  
Fares Hezam Al-Ostoot ◽  
Luc Van Meervelt ◽  
Sanae Lahmidi ◽  
...  

In the title molecule, C23H28N2O, the phenyl ring is inclined to the quinoxaline ring system at a dihedral angle of 20.40 (9)°. In the crystal, C—H...O interactions between neighbouring molecules form chains along the a-axis direction. Hirshfeld surface analysis indicates that the most important contributions to the crystal packing are from H...H (70.6%), H...C/C...H (15.5%) and H...O/O...H (4.6%) interactions. The optimized structure calculated using density functional theory at the B3LYP/6–311 G(d,p) level is compared with the experimentally determined structure in the solid state. The calculated highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) energy gap is 3.8904 eV. Part of the n-nonyl chain attached to one of the nitrogen atoms of the quinoxaline ring system shows disorder and was refined with a double conformation with occupancies of 0.604 (11) and 0.396 (11).


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