THE COORDINATION OF VO2+ TO HYDROXAMATE BINDERS AS STUDIED BY ORIENTATION SELECTIVE ESEEM SPECTROSCOPY

Citation
V. Kofman et al., THE COORDINATION OF VO2+ TO HYDROXAMATE BINDERS AS STUDIED BY ORIENTATION SELECTIVE ESEEM SPECTROSCOPY, Journal of the American Chemical Society, 117(1), 1995, pp. 383-391
Citations number
45
Categorie Soggetti
Chemistry
ISSN journal
00027863
Volume
117
Issue
1
Year of publication
1995
Pages
383 - 391
Database
ISI
SICI code
0002-7863(1995)117:1<383:TCOVTH>2.0.ZU;2-4
Abstract
The binding of VO2+ to chiral dihydroxamate binders facilitates the tr ansport of VO2+ through the cell membrane into the cell interior, wher e it was shown to simulate glucose metabolism (Shechter, Y;; Shisheva, A.; Lazar, R.; Libman, J.; Shanzer, A. Biochemistry 1992, 31, 2063). The unique structure of the binders relies on a modular dipodal topolo gy which generates different binding cavities. The coordination of VO2 + to two homologues of these ligands, RL261 and RL239, having differen t dipod arms but identical donor groups, was investigated by orientati on selective electron spin echo envelope modulation (ESEEM) spectrosco py. Relatively deep modulations were observed for the N-14 nuclei in t he hydroxamate groups in both complexes owing to the fulfillment of th e cancellation condition at similar to 9 GHz. The Fourier transform Fl ESEEM spectra showed four peaks, three corresponding to the nuclear q uadrupole resonance (NQR) lines, v(o), v(-), and v(+), and one to the overtone, 2(vm). In VO-RL261 the NQR and the 2(vm) peaks appear at 1.7 5, 2.15, 3.9, and 6.0 MHz, respectively, whereas in VO-RL239 they are at 1.75, 2.05, 3.9, and 6.2 MHz, respectively. From the positions of t hese peaks the N-14 quadrupole coupling constant, \e(2)qQ/h\, the asym metry parameter, eta, and the isotropic hyperfine constant \a(iso)\, w ere estimated to be 4.0, 0.87, and 2.5 MHz, respectively, for VO-RL261 and 3.8, 0.91, and 2.8 MHz, respectively, for VO-RL239. The unique or ientation dependence of the v(+) peak, which practically disappeared w hen the field was set to A(parallel to)(V-51), indicates that the prin cipal axis of the quadrupole tenser, z'', is either parallel or perpen dicular to the VO axis. In order to obtain more accurate values of the above parameters and to determine the anisotropic hyperfine component , a(perpendicular to), as well as the orientations of the hyperfine an d quadrupole tensors with respect to the VO axis, a series of simulati ons were carried out. The best fit parameters showed that a(perpendicu lar to) is rather large (0.6-0.7 MHz) and cannot be neglected and that a(iso) is smaller than expected, i.e., 1.6-1.8 MHz. We also obtained that z'' is to a good approximation parallel to the VO axis indicating that the two hydroxamate planes are perpendicular to the VO axis in b oth complexes. Two possible structures, one with a C-2 symmetry, trans configuration, and one with a sigma(xz) symmetry, cis configuration, were considered in the simulations and the latter was found to agree b etter with the experimental results. The slight differences in the par ameters obtained for VO-RL261 and VO-RL239 are attributed to electroni c effects induced by the different groups bounded to the hydroxamate c arbonyl.