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2 Homometallic Alkoxides

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96 Alkoxo and Aryloxo Derivatives of Metals<br />

thus interpreted in terms of an octahedrally coordinated cobalt(II) configuration in<br />

cobalt dimethoxide. The diffuse reflectance spectrum of cobalt chloride methoxide595 showed bands at 7300 cm 1 assigned to the 4 4 T1⊲F⊳ A2g transition and at 15 200,<br />

17 600, and 18 900, all being assigned to split 4 4 T1⊲P⊳ A2 transitions. Taking the<br />

value of 17 200 cm 1 , the average energy in this complex band gave the calculated<br />

values of 10 Dq D 4250 cm 1 and the Racah parameter B D 785 cm 1 which are<br />

comparable with the values observed for the CoCl4 2 ion (10 Dq D 3200 cm 1 and B D<br />

715 cm 1 ). 596 The higher values obtained for the chloride methoxide as compared with<br />

the CoCl4 2 ion may be attributed to the positions of methoxide ion and chloride ion in<br />

the spectrochemical series since the methoxide is at higher energy than the chloride. The<br />

above spectral data were consistent with the tetrahedral coordination of the Co(II) ion.<br />

The spectrum of cobalt bromide methoxide was also consistent with the tetrahedral<br />

configuration; however, on solvation with methanol to form CoBr(OMe).2MeOH<br />

a change from intense blue to pink with corresponding changes in the reflectance<br />

spectrum revealed a change in structure from tetrahedral to octahedral. 595<br />

The diffuse reflectance spectrum of cobalt iodide methoxide was rather complex and<br />

showed a large charge transfer band in the visible region. However, some discontinuity<br />

was observed around 16 000 and 18 000 cm 1 4 whichwasassignedtoa4T1⊲P⊳ A2<br />

transition superimposed on the charge transfer edge.<br />

The reflectance spectrum of the d8 nickel dimethoxide showed bands at 8700,<br />

14 500, and 25 000 cm 1 whichwereassignedto2 2 T2g⊲F⊳ A2g⊲F⊳, 3 3 T1g⊲F⊳ A2g,<br />

and 3 3 TIg⊲P⊳ A2g transitions, respectively. 219 The bands are in good agreement<br />

with the octahedral nickel(II) involving MO6 configuration. Nickel monochloride<br />

monomethoxide also exhibits three bands at 7900, 12 900 and 22 100 cm 1 with the<br />

ligand field parameter Dq D 790 and Racah parameter B D 870 in its reflectance<br />

spectrum which are consistent with octahedral geometry for the nickel(II) ion<br />

corresponding to 3 3<br />

T2g A2g, 3 3 T1g⊲F⊳ A2g, and 3 3 T1g⊲P⊳ A2g transitions,<br />

respectively. 541 The reflectance spectra of various halide alkoxides have also been<br />

measured, and show three bands at about the above positions. It was observed that<br />

in the series NiCl(OMe), NiCl(OMe).MeOH, Ni3Cl2⊲OMe⊳4, andNi3Cl⊲OMe⊳5 the<br />

3 3<br />

T2g A2g transition bands appear at 7900, 8100, 8200, and 8300 cm 1 , respectively<br />

which are consistent with the values 7200 and 8500 cm 1 observed for nickel dichloride<br />

and nickel dimethoxide, respectively. These observations indicate that the 10 Dq values<br />

increased steadily as chloride was replaced by methoxide in the above series.<br />

The diffuse reflectance spectrum of d9 copper dimethoxide showed broad asymmetric<br />

bands with a maximum in the range 13 800–16 000 cm 1 and these bands were assumed<br />

to be due to the 2 2<br />

T2g Eg transition. 542<br />

Karraker597 measured the electronic absorption spectrum of dimeric uranium pentaethoxide<br />

and the weak narrow bands observed at 5405, 5680, 6622, 6934, 10 200,<br />

11 690, and 14 490 cm 1 have been assigned to f–f transitions for a distorted octahedral<br />

f1 system with a spin–orbit coupling constant of 1905 cm 1 .<br />

3.6 Magnetic Susceptibility Measurements<br />

The magnetic properties of metal alkoxides have been studied in some detail for the<br />

first row transition metal alkoxides. Basi and Bradley 334 in 1963 measured the magnetic

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