H. Frydendahl et al., CHANGES IN GEOMETRIES AND SPIN STATES OF THIOLATO-SCHIFF BASE NIN2S2 COMPLEXES CONTAINING N,N'-BIPHENYL BACKBONES, Inorganic chemistry, 34(17), 1995, pp. 4467-4476
Four new 5-formylpyrazole-based thiolato Schiff base nickel(II) comple
xes (1-4) have been synthesized from the corresponding ligands and nic
kel(II) acetate. A new 2-mercaptobenzaldehyde Schiff base nickel(II) c
omplex (5) has been synthesized by two routes. X-ray structural analys
es on three of the complexes showed the following: 1, chemical formula
C26H26N6S2Ni, monoclinic, space group P2(1)/n with a = 10.438(2) Angs
trom, b = 12.450(3) Angstrom, c = 19.616(3) Angstrom, beta = 94.33(1)d
egrees, Z = 4, and R = 0.044 for 3365 reflections; 4, chemical formula
C34H26N6S2Ni, monoclinic, space group C2/c with a = 19.242(3) Angstro
m, b = 9.757(2) Angstrom, c = 19.691(3) Angstrom, beta = 125.84(1)degr
ees, Z = 4, and R = 0.032 for 2206 reflections; 5, chemical formula C2
8H22N2S2Ni, monoclinic, space group C2/c with a = 25.230(4) Angstrom,
b = 11.098(2) Angstrom, c = 17.287(8) Angstrom, beta = 98.46(3)degrees
, Z = 8, and R = 0.047 for 1912 reflections. The coordination geometry
in 1 is distorted tetrahedral while in 4 and 5 it is close to cis-squ
are planar despite the influence of the (6,6'-dimethyl)biphenyl group
in the tetradentate ligand backbone. The bond distances are as follows
. Ni-S: 1, 2.239(1), 2.243(1) Angstrom; 4, 2.185(1) Angstrom; 5, 2.152
(2), 2.184 (2) Angstrom. Ni-N: 1, 1.963(2), 1.968(2) Angstrom; 4, 1.92
7(2); 5, 1.931(5), 1.917(6) Angstrom. The distortions from tetrahedral
to planar geometry are manifest in some interesting changes in dihedr
al angles and donor atom ''bite'' distances. The magnetic susceptibili
ties were measured in the temperature range 4.2-300 K for 1-5. The sus
ceptibilities of 1 and 2 could be fitted well to a simple axial spin H
amiltonian with S = 1, D = 34 cm(-1) and S = 1, D = 53 cm(-1), respect
ively. Complexes 3-5 are diamagnetic and showed only small temperature
-independent paramagnetic susceptibilities. Although no temperature-in
duced spin changes were observed for solids of 1-4, they all showed a
(1)A(lg) reversible arrow T-3(1) equilibrium in chloroform solutions.
Each of complexes 1-5 show LF, CT, and intraligand spectral features i
n the spectral region 5,000 - 40,000 cm(-1). Bands assigned to the hig
h-spin and low-spin forms are observed separately. The thermodynamic p
arameters for the high-spin reversible arrow low-spin equilibria in ch
loroform solutions were obtained by using the Evans method, variable-t
emperature H-1 NMR spectra, and variable-temperature electronic spectr
a. Complexes 1-4 exhibit equilibrium constants K-eq (=N-HS/N-LS) in th
e range of 0.456-0.080.