TY - JOUR
T1 - Bis(bipyridine)-phenanthroline double-stranded helicates of the d10 metals
T2 - Zinc(II), silver(I) and copper(I) helicates
AU - Greenwald, Moshe
AU - Wessely, Dana
AU - Goldberg, Israel
AU - Cohen, Yoram
PY - 1999
Y1 - 1999
N2 - The new ligand 2,9-bis[(6-methyl-2,2'-bipyridin-6'- yl)methyleneoxymethylen-yl]-1,10-phenanthroline (1) was prepared and was shown to self-assemble into double-stranded helicates upon reaction with Cu+, Ag+ and Zn2+, thus affording the first trinuclear double-stranded zinc helicate. The [(1)2M3](3n+) [M = Cu+(n = 1), Ag+(n = 1) or Zn2+(n = 2)] helicates were characterized by 1D, 2D and diffusion NMR. FAB mass spectrometry corroborated the structure of the silver and the copper helicates and [(1)2Cu3]3+ was characterized by X-ray crystallography. The detailed assignments of the 1H NMR spectra of these helicates have shown that H-10 absorbs at a much higher field when compared to the other protons of these complexes. This high-field shift is a unique characteristic of the helicates of 1 and is not found in structurally related helicates. The NMR spectra of these helicates, at room temperature, are consistent with an average solution structure having a D2 symmetry. Variable-temperature 1H NMR (VT-NMR) reveals that the silver helicate of 1 is much more labile than its copper helicate. From the VT-NMR spectra it seems that two, nearly separate, stages are observed in the dissociation process of [(1)2Ag3]3+. The activation energy of the first process for [(1)2Ag3]3+ in DMSO-d6 was found to be 16.6 ± 0.2 kcal mol-1. As expected, the energy barriers for the respective copper helicate are even higher. The crystal structure of [(1)2Cu3]3+ shows that the total length and the pitch length are ≃17 and 12 Å, respectively.
AB - The new ligand 2,9-bis[(6-methyl-2,2'-bipyridin-6'- yl)methyleneoxymethylen-yl]-1,10-phenanthroline (1) was prepared and was shown to self-assemble into double-stranded helicates upon reaction with Cu+, Ag+ and Zn2+, thus affording the first trinuclear double-stranded zinc helicate. The [(1)2M3](3n+) [M = Cu+(n = 1), Ag+(n = 1) or Zn2+(n = 2)] helicates were characterized by 1D, 2D and diffusion NMR. FAB mass spectrometry corroborated the structure of the silver and the copper helicates and [(1)2Cu3]3+ was characterized by X-ray crystallography. The detailed assignments of the 1H NMR spectra of these helicates have shown that H-10 absorbs at a much higher field when compared to the other protons of these complexes. This high-field shift is a unique characteristic of the helicates of 1 and is not found in structurally related helicates. The NMR spectra of these helicates, at room temperature, are consistent with an average solution structure having a D2 symmetry. Variable-temperature 1H NMR (VT-NMR) reveals that the silver helicate of 1 is much more labile than its copper helicate. From the VT-NMR spectra it seems that two, nearly separate, stages are observed in the dissociation process of [(1)2Ag3]3+. The activation energy of the first process for [(1)2Ag3]3+ in DMSO-d6 was found to be 16.6 ± 0.2 kcal mol-1. As expected, the energy barriers for the respective copper helicate are even higher. The crystal structure of [(1)2Cu3]3+ shows that the total length and the pitch length are ≃17 and 12 Å, respectively.
UR - http://www.scopus.com/inward/record.url?scp=0032794134&partnerID=8YFLogxK
U2 - 10.1039/a808673g
DO - 10.1039/a808673g
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AN - SCOPUS:0032794134
SN - 1144-0546
VL - 23
SP - 337
EP - 344
JO - New Journal of Chemistry
JF - New Journal of Chemistry
IS - 3
ER -