| Literature DB >> 28230756 |
Matija Uršič1, Tanja Lipec2, Anton Meden3, Iztok Turel4.
Abstract
Four novel ruthenium organometallic complexes: [(η⁶-p-cymene)Ru(4,4,4-trifluoro-1-(4-bromophenyl)-1,3-butanedione)Cl] (1), [(η⁶-p-cymene)Ru(4,4,4-trifluoro-1-(4-bromophenyl)-1,3-butanedione)pta]PF₆ (2), [(η⁶-p-cymene)Ru(4,4,4-trifluoro-1-(4-iodophenyl)-1,3-butanedione)Cl] (3) and [(η⁶-p-cymene)Ru(4,4,4-trifluoro-1-(4-iodophenyl)-1,3-butanedione)pta]PF₆ (4) were synthesized and characterized by elemental analysis, infrared (IR), UV-Vis, NMR and mass spectroscopy and single-crystal X-ray diffraction. The crystal structures and spectroscopic data were compared to the previously published complexes [(η⁶-p-cymene)Ru(4,4,4-trifluoro-1-(4-chloro-phenyl)-1,3-butanedione)Cl] (5) and [(η⁶-p-cymene)Ru(4,4,4-trifluoro-1-(4-chlorophenyl)-1,3-butanedione)pta]PF₆ (6). The pairs of complexes 1 and 3 as well as 2 and 4 are isostructural, with the former crystallizing in triclinic P-1 and the latter in monoclinic P2₁/c. The ruthenium(II) ion is found in a pseudo-octahedral "piano-stool" geometry in all compounds. Bond lengths and angles are consistent with other complexes of this type. Complexes 2 and 4 exhibit some moderate dynamic disorder. The lack of hydrogen bonding and major π-π interactions means that most of intramolecular interactions are fairly weak and involve halogen atoms present. This was further confirmed by ¹H-NMR spectra, where a significant difference is observed only on the ligand near the halogen atom, following an expected trend. The combined data show that the difference in any activity depends substantially on the type of the ligand's substituted halogen atom.Entities:
Keywords: 1,3,5-triazaphosphoadamantane (pta) ligand; disorder; halogen substituents; organoruthenium complexes; β-diketonate ligands
Mesh:
Substances:
Year: 2017 PMID: 28230756 PMCID: PMC6155601 DOI: 10.3390/molecules22020326
Source DB: PubMed Journal: Molecules ISSN: 1420-3049 Impact factor: 4.411
Figure 1General structure of the studied complexes with the crystallographic atom numbering scheme, used throughout this text.
Figure 2Asymmetric unit of 3. Thermal ellipsoids are drawn at 30% probability. Hydrogen atoms are omitted for clarity. Compounds 1 and 3 are isostructural.
Figure 3Asymmetric unit of 4. Thermal ellipsoids are drawn at 30% probability. Hydrogen atoms and atoms introduced to model disorder are omitted for clarity. Compounds 2 and 4 are isostructural.
Selected bond lengths (Å) and angles (°) in the studied compounds 1–6. All bond lengths and angles for compounds 1–4 can be found in supplementary information in respective tables.
| Bond/Angle | 1 | 3 | 5 | 2 | 4 | 6 |
|---|---|---|---|---|---|---|
| Ru1–O17 | 2.096(3) | 2.097(4) | 2.091(2) | 2.081(8) | 2.081(7) | 2.094(4) |
| Ru1’–O17’ | 2.095(3) | 2.099(4) | / | / | / | |
| Ru1–O20 | 2.081(3) | 2.079(3) | 2.092(1) | 2.074(8) | 2.074(6) | 2.072(4) |
| Ru1’–O20’ | 2.076(2) | 2.088(4) | / | / | / | / |
| Ru1–Cl1 | 2.393(1) | 2.396(1) | 2.405(1) | / | / | / |
| Ru1’–Cl1’ | 2.394(1) | 2.397(1) | / | / | / | / |
| Ru1–P30 | / | / | / | 2.318(2) | 2.314(2) | 2.3270(7) |
| O17–Ru1–O20 | 87.7(1) | 88.1(2) | 87.44(3) | 87.6(3) | 87.6(2) | 87.44(7) |
| O17’–Ru1’–O20’ | 87.3(1) | 88.0(2) | / | / | / | / |
Figure 4Interaction between the bromine atom and phenyl ring in 1. Thermal ellipsoids drawn at 30% probability. Centroid to halogen atom distances: 1: 3.772 Å; 3: 3.807 Å.
Figure 5Weak interactions in 1 with the participating non-hydrogen atoms labelled. Thermal ellipsoids drawn at 30% probability. Hydrogen atoms not participating in marked interactions omitted for clarity.
Figure 6Disorder in 2 (left) and 4 (right). Darkness indicates overlap between two possible structures, black meaning complete overlap. Hydrogen atoms omitted for clarity. Thermal ellipsoids at 50% probability. Occupancy ratios: 2—0.659/0.341, 4—0.777/0.223.
Crystal data of complexes 1–6.
| Complex Number | 1 | 2 | 3 | 4 |
|---|---|---|---|---|
| Empirical formula | C20H19BrClF3O2Ru | C26H31BrF9N3O2P2Ru | C20H19ClF3IO2Ru | C26H31F9IN3O2P2Ru |
| Formula weight | 564.78 | 831.46 | 611.77 | 878.45 |
| Temperature/K | 150.00(10) | 150.00(10) | 150.00(10) | 150.00(10) |
| Crystal system | triclinic | monoclinic | triclinic | monoclinic |
| Space group | P-1 | P21/c | P-1 | P21/c |
| a/Å | 10.0249(4) | 10.6584(5) | 9.9973(3) | 10.6889(4) |
| b/Å | 12.9431(6) | 14.8139(6) | 12.9283(5) | 14.8208(5) |
| c/Å | 18.0374(7) | 19.6695(8) | 18.2806(8) | 19.8820(6) |
| α/° | 72.014(4) | 90 | 71.413(4) | 90 |
| β/° | 80.020(3) | 94.661(4) | 80.368(3) | 93.538(3) |
| γ/° | 76.696(4) | 90 | 76.830(3) | 90 |
| Volume/Å3 | 2153.05(17) | 3095.4(2) | 2169.09(14) | 3143.65(17) |
| Z | 4 | 4 | 4 | 4 |
| ρcalc·g/cm3 | 1.742 | 1.784 | 1.873 | 1.856 |
| μ/mm−1 | 2.746 | 1.986 | 18.506 | 1.666 |
| F (000) | 1112.0 | 1656.0 | 1184.0 | 1728.0 |
| Radiation | Mo Kα (λ = 0.7107) | Mo Kα (λ = 0.7107) | Cu Kα (λ = 1.5418) | Mo Kα (λ = 0.7107) |
| Reflections collected | 16,610 | 17,899 | 15,274 | 20,267 |
| Independent reflections | 9837 (Rint = 0.0328, Rsigma = 0.0668) | 8116 (Rint = 0.0400, Rsigma = 0.0660) | 8508 (Rint = 0.0529, Rsigma = 0.0637) | 8291 (Rint = 0.0345, Rsigma = 0.0529) |
| Data/restraints/parameters | 9837/0/509 | 8116/0/440 | 8508/0/511 | 8291/0/410 |
| Goodness-of-fit on F2 | 1.007 | 1.031 | 1.040 | 1.030 |
| Final R indexes (I ≥ 2σ (I)) | R1 = 0.0445, wR2 = 0.0909 | R1 = 0.0665, wR2 = 0.1699 | R1 = 0.0445, wR2 = 0.1217 | R1 = 0.0532, wR2 = 0.1059 |
| Final R indexes (all data) | R1 = 0.0753, wR2 = 0.1027 | R1 = 0.1132, wR2 = 0.1942 | R1 = 0.0548, wR2 = 0.1325 | R1 = 0.0869, wR2 = 0.1207 |
| Largest diff. peak/hole/e Å−3 | 0.94/−1.03 | 1.64/−0.89 | 1.59/−1.29 | 1.55/−0.73 |
Scheme 1General scheme for two-step preparation of complexes.