| Literature DB >> 24819403 |
David W Boyce1, Debra J Salmon, William B Tolman.
Abstract
The synthesis of a series of asymmetric mixed 2,6-disubstituted (arylcarboxamido)(arylimino)pyridine ligands and theirEntities:
Mesh:
Substances:
Year: 2014 PMID: 24819403 PMCID: PMC4045151 DOI: 10.1021/ic500638z
Source DB: PubMed Journal: Inorg Chem ISSN: 0020-1669 Impact factor: 5.165
Scheme 1
Figure 1Representations of the X-ray crystal structures of (a) L(H) (2c), (b) LCuCl (8b), (c) Me2LCuCl (8a), and (d) LCuOAc (9b), showing all non-hydrogen atoms as 50% thermal ellipsoids. See Table 1 for selected interatomic distances and angles.
Selected Interatomic Distances (Å) and Angles (deg) for the Indicated X-ray Crystal Structuresa
| Me2LCuCl ( | |||||||
|---|---|---|---|---|---|---|---|
| N(1)–C(1) | 1.344(3) | O(1)–C(1)–N(1) | 124.0(3) | Cu(1)–N(1) | 2.005(3) | N(2)–Cu(1)–N(1) | 80.18(12) |
| O(1)–C(1) | 1.223(3) | N(1)–C(1)–C(3) | 114.2(2) | Cu(1)–N(2) | 1.934(3) | N(2)–Cu(1)–N(3) | 77.58(11) |
| C(2)–N(3) | 1.260(3) | N(3)–C(2)–C(8) | 126.6(2) | Cu(1)–N(3) | 2.130(3) | N(1)–Cu(1)–N(3) | 154.56(11) |
| C(2)–N(3)–C(21) | 122.6(2) | Cu(1)–Cl(1) | 2.2092(10) | N(2)–Cu(1)–Cl(1) | 172.53(9) | ||
| Cu(1)–O(1)′ | 2.345(3) | N(1)–Cu(1)–Cl(1) | 102.41(9) | ||||
| N(3)–Cu(1)–Cl(1) | 98.25(8) | ||||||
Estimated standard deviations are indicated in parentheses. Full lists of atomic coordinates and bond distances are available in the CIFs (Supporting Information).
Scheme 2
Figure 2EPR spectra (black) and simulations (gray) of (a) Me2LCuCl (8a) and (b) LCuCl (8b). Parameters derived from the simulations are listed in Table 2.
EPR Parameters Derived from Simulations of Experimental X-Band Spectraa
| entry | compound | ref | ||||||
|---|---|---|---|---|---|---|---|---|
| 1 | Me2LCuCl ( | 2.08 | 2.05 | 2.23 | 165 | 12.5 | 12.5 | |
| 2 | 2.065 | 2.09 | 2.20 | 196 | 15 | 15 | ||
| 3 | 2.06 | 2.045 | 2.185 | 197 | 15 | 15 | ||
| 4 | 2.037 | 2.072 | 2.21 | 190 | 15 | |||
| 5 | 2.07 | 2.055 | 2.20 | 194 | 15 | |||
| 6 | ( | 2.027 | 2.064 | 2.190 | 199 | 15.6 | ( | |
| 7 | ( | 2.028 | 2.055 | 2.189 | 193 | 15 | ( | |
| 8 | [ | 2.06 | 2.07 | 2.27 | 165 | |||
| 9 | [ | 2.06 | 2.07 | 2.27 | 165 | |||
| 10 | [ | 2.03 | 2.11 | 2.27 | 155 | |||
| 11 | 2.14 | 2.14 | 2.14 |
Measured in frozen solution at 2–30 K; units of A are in 10–4 cm–1. See the Experimental Section or indicated references for details.
This work.
Figure 3Cyclic voltammograms of [(1)CuCl]– (black trace) and LCuCl (8b) (red trace) all performed in acetone (0.1 M Bu4NPF6).
Scheme 3
Figure 5Representations of the X-ray crystal structures of (a) L(H)ZnCl2 (15), (b) [L(H)Cu(MeCN)][(SbF6)2] (10), and (c) [L(H)CuOH2(THF)](SbF6)2 (12) (omitting one SbF6– and showing two additional THF solvate molecules), with all non-hydrogen atoms shown as 50% thermal ellipsoids and the hydrogen atoms attached to the amide N atoms and the H2O molecule as spheres. See Table 1 for selected interatomic distances and angles.
Figure 4EPR spectra (black) and simulations (gray) of (a) LCuOAc (9c) and (b) [L(H)Cu(MeCN)2][(SbF6)2] (11). Parameters derived from the simulations are listed in Table 2.