5852 Inorganic Chemistry, Vol. 37, No. 22, 1998
Cornman et al.
Table 1. Crystallographic Data for K[MoVIO2(btap)], 1, and
Experimental Procedures
[NiII(Hbtap)]2, 2
Materials were purchased from commercial sources and used as
received unless otherwise stated. Dry solvents were prepared by
distillation from CaH2 (acetonitrile and hexanes), diphenylketyl radical
(THF), or Mg(OMe)2 (methanol) under dinitrogen.22,23 Acetone was
dried via passage through Al2O3.
1
2
empirical formula
fw
temperature
space group
C11H16NO4S2KMo
425.41
C24H38N2O4S4Ni
664.22
148 K
Pbcn
133 K
Pbcn
Bis(2-mercaptoethyl)-2-amino-4-methylphenol (H3btap). Ethyl-
ene sulfide (14 mL, 0.12 mol) was added to a refluxing toluene solution
(50 mL) of 2-amino-4-methylphenol (5.36 g, 43.5 mmol). The reaction
was heated for 40 h at 90 °C. The resulting brownish solution was
concentrated to 3 mL in Vacuo, transferred to a silica gel column, and
eluted with a 1:9:27 MeOH/CH2Cl2/hexanes solution. The clear, faintly
orange fraction was stripped of solvent via rotary evaporation, checked
for purity by 1H NMR and used without further purification. 1H NMR
(DMSO-d6) δ (ppm): 2.19 (s, 3 H), 2.49 (under solvent, m, 4 H), 3.16
(m, 4 H), 6.68 (s, 2 H), 6.83 (s, 1 H).
K[MoVIO2(btap)], 1. Mo(acac)2 (0.32 g, 0.98 mmol) was added to
a solution of KOH (0.055 g, 0.98 mmol) and H3btap (0.24 g, 0.98 mmol)
in 100 mL of methanol. This solution was stirred for 40 min and
filtered, and the solvent was removed under vacuum. The resulting
solid was dissolved in acetone and the residual particulate matter was
removed by filtration. Addition of hexanes and evaporation under
vacuum yielded 1 as an orange solid in 65% yield. X-ray-quality
crystals of 1 were obtained by slow evaporation of an acetone/hexanes
solution of 1. 1H NMR (see Figure S3, acetone-d6) δ (ppm) for 1:
2.93 (s, 3H), 3.09 (m, 4H), 3.65 (d of d, 2H), 4.25 (m, 2H), 6.34 (d,
1H), 6.58 (d, 1H), 6.76 (s, 1H). The resonance at δ ) 2.93 ppm is
assigned to the p-methyl protons. The resonances between δ ) 3.09
and 4.25 ppm are assigned to the diastereotopic methylene protons of
the thioethyl arms and the resonances at δ ) 6.34, 6.58, and 6.76 ppm
are assigned to the aromatic ring protons.
[NiII(Hbtap)]2, 2. Under an dinitrogen atmosphere, Ni(OAc)2‚4H2O
(215 mg, 0.862 mmol) was added to a 25 mL solution of acetonitrile
containing excess H3btap (236 mg, 0.951 mmol). The light brown
solution was stirred for 3 h to produce a fine brown precipitate of 2 in
79% yield. Red/brown X-ray-quality crystals were grown by slow
evaporation of a MeOH solution. 1H NMR (see Figure 3; 9:1 CH2-
Cl2/DMSO-d6) δ (ppm) for 2: 1.13 (t of d, 2H), 1.68 (d of d, 2H),
2.02 (d of d, 2H), 2.28 (t, 2H), 2.39 (s, 6H), 3.67 (t of d, 2H), 3.87 (d,
2H), 4.39 (d of d, 2H), 5.16 (t of d, 2H), 6.65 (d, 2H), 6.91 (d, 2H),
9.40 (s, 2H), 10.57 (s, 2H). The multiplets between δ ) 1.13 and 516
ppm are assigned to the methylene protons of the thioethyl groups.
The resonance at δ ) 2.39 ppm is assigned to the para-methyl protons.
The resonances at δ ) 6.65, 6.91, and 9.40 ppm are assigned the
phenolic ring protons, and the resonance at δ ) 10.57 ppm is assigned
to phenolic proton.
a (Å)
6.6596(9)
13.7446(9)
32.992(2)
90, 90, 90
3019.9(5)
1.871
12.0841(3)
14.4948(4)
16.7751(4)
90, 90, 90
2938.27(13)
1.502
b (Å)
c (Å)
R, â, γ (deg)
V (Å3)
F
Z
calc (g cm-3
)
8
4
λ (Mo KR) (Å)
0.710 73
1.40
0.710 73
1.598
0.0493
0.0697
µ (mm-1
)
R1a (all data)
wR2b (all data)
Rc [I > 1σ(I)]
Rwd [I > 1σ(I)]
0.041
0.049
a R1 ) ∑||Fo| - |Fc||/∑|Fo|. b (∑[w(Fo - Fc2)2]/∑[wFo ])1/2
.
c R )
2
4
2
∑(Fo - Fc)/∑(Fo). d Rw ) [∑(w(Fo - Fc)2)/∑(wFo )]1/2
.
set of programs.24 The structure was solved using SIR92.25 All non-H
atom positions were recovered from the initial E map. Subsequent
difference Fourier maps yielded peaks suggestive of hydrogen atom
positions, however, hydrogen atoms were added at their idealized
positions (C-H ) 0.96 Å). The phenyl and methylene hydrogens were
allowed to ride the parent carbon atom, while the methyl hydrogens
and the hydrogens on the water molecule were included as rigid groups.
Hydrogen isotropic displacement parameters rode on the parent carbon
atom’s Ueq value according to the expression U(H) ) U(C) + 0.01 Å2.
All non-H atoms were allowed to refine with anisotropic displacement
parameters. The calculated structure factors included corrections for
anomalous dispersion from the usual tabulation.26 The final full-matrix
least-squares refinement (based on F) converged at RF ) 0.041, Rw
)
0.049 (for data Inet > 1σ(Inet)). The largest peak in the final difference
map was 0.720 e/Å3. Selected distances and angles for 1 are given in
Table 2.
Structural determination for 2 was performed using a Siemens
SMART CCD-based X-ray diffractometer equipped with a normal focus
Mo-target X-ray tube (λ ) 0.710 73 Å) operated at 2000 W power (50
kV, 40 mA). X-ray intensities were measured at 133 K and the frames
integrated with the Siemens SAINT software package with a narrow
frame algorithm. The integration of the data using a primitive
orthorhombic unit cell yielded a total of 30307 reflections (between
2.19 e 2θ e 58.82°) of which 4312 were independent and 3269 were
greater than 2σ(I). The final cell constants (Table 1) were based on
the xyz centroids of 8192 reflections above 10σ(I). Analysis of the
data showed negligible decay during data collection; the data were
corrected for absorption using an empirical method (SADABS) with
transmission coefficients ranging from 0.825 to 0.962. The structure
of 2 was solved and refined with the Siemens SHELXTL (version 5.03)
software package, using the space group Pbcn with Z ) 4 for the
formula C24H38N2O4S4Ni which includes one molecule of methanol
solvate per asymmetric unit (2 per Ni dimer). All non-hydrogen atoms
were refined anisotropically while the hydrogen atoms were allowed
to refine isotropically. The final full-matrix least-squares refinement
based on F2 converged at R1 ) 0.0493 and wR2 ) 0.0697 (for all data);
the largest peak in the final difference map was 0.0434 e/Å3. Selected
distances and angles for 2 are given in Table 3.
Physical Measurements. 1H NMR spectra were obtained using a
General Electric GN 300 spectrometer using residual solvent protons
as an internal reference. UV/vis data were collected on a Hewlett-
Packard 8452A diode array spectrophotometer. Infrared spectra were
obtained on a Mattson Polaris spectrometer.
X-ray Crystal Structure Analysis. Crystallographic data for 1 and
2 are shown in Table 1. Structural determination for K[MoVIO2(btap)],
1, was performed using an Enraf-Nonius CAD4-MACH diffractometer.
The sample was maintained at a temperature of 148 K using a nitrogen
cold stream. The unit cell dimensions were determined by a fit of 24
well-centered reflections and their Friedel pairs with 28 < 2θ < 38°.
A unique octant (+h, +k, +l) of data was collected using the omega
scan mode in a nonbisecting geometry (3.0 e 2θ e 50.0°). Three
standard reflections were measured every 4800 s of X-ray exposure
time. Scaling the data was accomplished using a five-point smoothed-
curve routine fit to the intensity check reflections. The intensity data
was corrected for Lorentz and polarization effects. An empirical
absorption correction based on psi scans was applied during data
reduction. The data were reduced using routines from the NRCVAX
Results and Discussion
Structures. In the vanadium(V) complex of H3btap, the
ligand adopts a tetradentate, tripodal coordination mode to give
(24) Gabe, E. J.; Le Page, Y.; Charland, J.-P.; Lee, F. L.; White, P. S. J.
Appl. Crystallogr. 1989, 22, 384-387.
(25) Altomare, A.; Burla, M. C.; Camalli, G.; Cascarano, G.; Giacovazzo,
C.; Gualiardi, A.; Polidori, G. J. Appl. Crystallogr. 1994, 27, 435-
436.
(22) Gordon, A. J.; Ford, R. A. The Chemist’s Companion; John Wiley &
Sons: New York, 1972.
(23) Armarego, W. L. F.; Perrin, D. D. Purification of Laboratory
Chemicals, 4th ed.; Butterworth-Heinemann: Oxford, 1996.
(26) International Tables for X-ray Crystallography; Ibers, J., Hamilton,
W., Ed.; Kynoch Press: Birmingham, England, 1974; Vol. IV.