Crystal structure determination, and DFT Calculations of dichlorobis-(dimethylsulfoxide-O)copper(II)
- Authors: Chebbi H.1,2, Chebbi M.3, Guesmi A.2, Arfaoui Y.3
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Affiliations:
- Preparatory Institute in the Studies of Engineers of Monastir
- Laboratory of Materials and Crystallochemistry, Department of Chemistry, Faculty of Science
- Laboratory of Physical Chemistry of Condensed Materials, Department of Chemistry, Faculty of Science
- Issue: Vol 57, No 6 (2016)
- Pages: 1104-1110
- Section: Article
- URL: https://journals.rcsi.science/0022-4766/article/view/160766
- DOI: https://doi.org/10.1134/S002247661606007X
- ID: 160766
Cite item
Abstract
The crystal structure of dichlorobis(dimethylsulfoxide-O)copper(II), [CuCl2(DMSO)2] (I), previously determined by Willett and Chang, is reinvestigated. It crystallizes in the orthorhombic system with the space group Pnma (N°62), Z = 4, and unit cell parameters a = 8.053(1) Å, b = 11.642(5) Å, c = 11.347(3) Å. Our structure determination is of a significantly higher precision in terms of bond lengths, angles, and R factors (e.g., Cu1–O1 = 1.9737(24) Å, O1–Cu1–O1i = 173.08(13)° (symmetry code: Ix, 1/2–y, z) and R(F2) = 0.046 compared to 1.955(4) Å, 173.0(3)° and R(F) = 0.075). In contrast to the previous investigation, all H atoms are placed at calculated positions. In the title molecule, the CuII atom is five coordinated in a distorted square pyramidal geometry. Thus, as reported previously, it can be shown that the crystal structure consists of [CuCl2(DMSO)2] molecules which, by virtue of long Cu–Cl interactions, are tied together to form chains parallel to the [100] direction. The density functional theory (DFT) optimized structure at the B3LYP/6-311++G(2d,2p) level is compared with the experimentally determined molecular structure. The HOMO-LUMO energy gap and other related molecular properties are also calculated. Comprehensive experimental and theoretical structural studies on the studied complex are carried out by FT-IR and UV-visible spectroscopies.
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About the authors
H. Chebbi
Preparatory Institute in the Studies of Engineers of Monastir; Laboratory of Materials and Crystallochemistry, Department of Chemistry, Faculty of Science
Email: chebhamouda@yahoo.fr
Tunisia, Tunisia; Tunisia
M. Chebbi
Laboratory of Physical Chemistry of Condensed Materials, Department of Chemistry, Faculty of Science
Author for correspondence.
Email: chebhamouda@yahoo.fr
Tunisia, Tunisia, 2092
A. Guesmi
Laboratory of Materials and Crystallochemistry, Department of Chemistry, Faculty of Science
Email: chebhamouda@yahoo.fr
Tunisia, Tunisia
Y. Arfaoui
Laboratory of Physical Chemistry of Condensed Materials, Department of Chemistry, Faculty of Science
Email: chebhamouda@yahoo.fr
Tunisia, Tunisia, 2092
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