Cargando…

Crystal structure, Hirshfeld surface and crystal void analysis, inter­molecular inter­action energies, DFT calculations and energy frameworks of 2H-benzo[b][1,4]thia­zin-3(4H)-one 1,1-dioxide

In the title mol­ecule, C(8)H(7)NO(3)S, the nitro­gen atom has a planar environment, and the thia­zine ring exhibits a screw-boat conformation. In the crystal, corrugated layers of mol­ecules parallel to the ab plane are formed by N—H⋯O and C—H⋯O hydrogen bonds together with C—H⋯π(ring) and S=O⋯π(ri...

Descripción completa

Detalles Bibliográficos
Autores principales: Irrou, Ezaddine, Ait Elmachkouri, Younesse, Mazzah, Ahmed, Hökelek, Tuncer, Haoudi, Amal, Mague, Joel T., Taha, Mohamed Labd, Sebbar, Nada Kheira
Formato: Online Artículo Texto
Lenguaje:English
Publicado: International Union of Crystallography 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10626949/
https://www.ncbi.nlm.nih.gov/pubmed/37936855
http://dx.doi.org/10.1107/S205698902300868X
_version_ 1785131438032551936
author Irrou, Ezaddine
Ait Elmachkouri, Younesse
Mazzah, Ahmed
Hökelek, Tuncer
Haoudi, Amal
Mague, Joel T.
Taha, Mohamed Labd
Sebbar, Nada Kheira
author_facet Irrou, Ezaddine
Ait Elmachkouri, Younesse
Mazzah, Ahmed
Hökelek, Tuncer
Haoudi, Amal
Mague, Joel T.
Taha, Mohamed Labd
Sebbar, Nada Kheira
author_sort Irrou, Ezaddine
collection PubMed
description In the title mol­ecule, C(8)H(7)NO(3)S, the nitro­gen atom has a planar environment, and the thia­zine ring exhibits a screw-boat conformation. In the crystal, corrugated layers of mol­ecules parallel to the ab plane are formed by N—H⋯O and C—H⋯O hydrogen bonds together with C—H⋯π(ring) and S=O⋯π(ring) inter­actions. The layers are connected by additional C—H⋯O hydrogen bonds and π-stacking inter­actions. Hirshfeld surface analysis indicates that the most important contributions for the crystal packing are from H⋯O/O⋯H (49.4%), H⋯H (23.0%) and H⋯C/C⋯H (14.1%) inter­actions. The volume of the crystal voids and the percentage of free space were calculated as 75.4 Å(3) and 9.3%. Density functional theory (DFT) computations revealed N—H⋯O and C—H⋯O hydrogen-bonding energies of 43.3, 34.7 and 34.4 kJ mol(−1), respectively. Evaluation of the electrostatic, dispersion and total energy frameworks indicate that the stabilization is dominated via the electrostatic energy contribution. Moreover, the DFT-optimized structure at the B3LYP/ 6–311 G(d,p) level is compared with the experimentally determined mol­ecular structure in the solid state. The HOMO–LUMO behaviour was elucidated to determine the energy gap.
format Online
Article
Text
id pubmed-10626949
institution National Center for Biotechnology Information
language English
publishDate 2023
publisher International Union of Crystallography
record_format MEDLINE/PubMed
spelling pubmed-106269492023-11-07 Crystal structure, Hirshfeld surface and crystal void analysis, inter­molecular inter­action energies, DFT calculations and energy frameworks of 2H-benzo[b][1,4]thia­zin-3(4H)-one 1,1-dioxide Irrou, Ezaddine Ait Elmachkouri, Younesse Mazzah, Ahmed Hökelek, Tuncer Haoudi, Amal Mague, Joel T. Taha, Mohamed Labd Sebbar, Nada Kheira Acta Crystallogr E Crystallogr Commun Research Communications In the title mol­ecule, C(8)H(7)NO(3)S, the nitro­gen atom has a planar environment, and the thia­zine ring exhibits a screw-boat conformation. In the crystal, corrugated layers of mol­ecules parallel to the ab plane are formed by N—H⋯O and C—H⋯O hydrogen bonds together with C—H⋯π(ring) and S=O⋯π(ring) inter­actions. The layers are connected by additional C—H⋯O hydrogen bonds and π-stacking inter­actions. Hirshfeld surface analysis indicates that the most important contributions for the crystal packing are from H⋯O/O⋯H (49.4%), H⋯H (23.0%) and H⋯C/C⋯H (14.1%) inter­actions. The volume of the crystal voids and the percentage of free space were calculated as 75.4 Å(3) and 9.3%. Density functional theory (DFT) computations revealed N—H⋯O and C—H⋯O hydrogen-bonding energies of 43.3, 34.7 and 34.4 kJ mol(−1), respectively. Evaluation of the electrostatic, dispersion and total energy frameworks indicate that the stabilization is dominated via the electrostatic energy contribution. Moreover, the DFT-optimized structure at the B3LYP/ 6–311 G(d,p) level is compared with the experimentally determined mol­ecular structure in the solid state. The HOMO–LUMO behaviour was elucidated to determine the energy gap. International Union of Crystallography 2023-10-19 /pmc/articles/PMC10626949/ /pubmed/37936855 http://dx.doi.org/10.1107/S205698902300868X Text en © Irrou et al. 2023 https://creativecommons.org/licenses/by/4.0/This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
spellingShingle Research Communications
Irrou, Ezaddine
Ait Elmachkouri, Younesse
Mazzah, Ahmed
Hökelek, Tuncer
Haoudi, Amal
Mague, Joel T.
Taha, Mohamed Labd
Sebbar, Nada Kheira
Crystal structure, Hirshfeld surface and crystal void analysis, inter­molecular inter­action energies, DFT calculations and energy frameworks of 2H-benzo[b][1,4]thia­zin-3(4H)-one 1,1-dioxide
title Crystal structure, Hirshfeld surface and crystal void analysis, inter­molecular inter­action energies, DFT calculations and energy frameworks of 2H-benzo[b][1,4]thia­zin-3(4H)-one 1,1-dioxide
title_full Crystal structure, Hirshfeld surface and crystal void analysis, inter­molecular inter­action energies, DFT calculations and energy frameworks of 2H-benzo[b][1,4]thia­zin-3(4H)-one 1,1-dioxide
title_fullStr Crystal structure, Hirshfeld surface and crystal void analysis, inter­molecular inter­action energies, DFT calculations and energy frameworks of 2H-benzo[b][1,4]thia­zin-3(4H)-one 1,1-dioxide
title_full_unstemmed Crystal structure, Hirshfeld surface and crystal void analysis, inter­molecular inter­action energies, DFT calculations and energy frameworks of 2H-benzo[b][1,4]thia­zin-3(4H)-one 1,1-dioxide
title_short Crystal structure, Hirshfeld surface and crystal void analysis, inter­molecular inter­action energies, DFT calculations and energy frameworks of 2H-benzo[b][1,4]thia­zin-3(4H)-one 1,1-dioxide
title_sort crystal structure, hirshfeld surface and crystal void analysis, inter­molecular inter­action energies, dft calculations and energy frameworks of 2h-benzo[b][1,4]thia­zin-3(4h)-one 1,1-dioxide
topic Research Communications
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10626949/
https://www.ncbi.nlm.nih.gov/pubmed/37936855
http://dx.doi.org/10.1107/S205698902300868X
work_keys_str_mv AT irrouezaddine crystalstructurehirshfeldsurfaceandcrystalvoidanalysisintermolecularinteractionenergiesdftcalculationsandenergyframeworksof2hbenzob14thiazin34hone11dioxide
AT aitelmachkouriyounesse crystalstructurehirshfeldsurfaceandcrystalvoidanalysisintermolecularinteractionenergiesdftcalculationsandenergyframeworksof2hbenzob14thiazin34hone11dioxide
AT mazzahahmed crystalstructurehirshfeldsurfaceandcrystalvoidanalysisintermolecularinteractionenergiesdftcalculationsandenergyframeworksof2hbenzob14thiazin34hone11dioxide
AT hokelektuncer crystalstructurehirshfeldsurfaceandcrystalvoidanalysisintermolecularinteractionenergiesdftcalculationsandenergyframeworksof2hbenzob14thiazin34hone11dioxide
AT haoudiamal crystalstructurehirshfeldsurfaceandcrystalvoidanalysisintermolecularinteractionenergiesdftcalculationsandenergyframeworksof2hbenzob14thiazin34hone11dioxide
AT maguejoelt crystalstructurehirshfeldsurfaceandcrystalvoidanalysisintermolecularinteractionenergiesdftcalculationsandenergyframeworksof2hbenzob14thiazin34hone11dioxide
AT tahamohamedlabd crystalstructurehirshfeldsurfaceandcrystalvoidanalysisintermolecularinteractionenergiesdftcalculationsandenergyframeworksof2hbenzob14thiazin34hone11dioxide
AT sebbarnadakheira crystalstructurehirshfeldsurfaceandcrystalvoidanalysisintermolecularinteractionenergiesdftcalculationsandenergyframeworksof2hbenzob14thiazin34hone11dioxide