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K.A.N.S. Ariyaratne et al. / Journal of Organometallic Chemistry 689 (2004) 2029–2032
sodium-benzophenone and were distilled prior to use.
Cp*2UCl2 was prepared using a literature method [16]
and HNSPh2 ꢀ H2O was purchased from Aldrich chem-
ical company. Cp*2UCl2(HNSPh2) was synthesized by
the reaction of Cp*2UCl2 with anhydrous HNSPh2 [14].
1H NMR spectra were obtained using a Nicolet QE 300
MHz spectrometer and samples were prepared in d6-
benzene, d8-toluene or d8-tetrahydrofuran. IR spectra
were recorded on a Perkin Elmer 1430 spectrometer or a
Nicolet-740 IR spectrometer operating in the Fourier
transform mode.
polarization effects and for decay of the intensities of
check reflections during data collection and an empirical
absorption correction was applied. The position of the
uranium was determined by direct methods and the re-
maining atoms were located in subsequent rounds of
difference Fourier maps and least squares refinements.
All non-hydrogen atoms were refined anisotropically
with restraints applied to non-U atoms. After an empir-
ical absorption correction, the H atoms were added at
calculated positions to the Cpꢁ methyl groups, phenyl
groups and the two benzene solvate molecules. The final
refinement yielded R values, R1 ¼ 6:51%, wR2 ¼ 16:30%
(I > 2rðIÞ and R ¼ 9:81%, wR2 ¼ 18:45% (all data)).
Crystalline Cp*2UCl(OH)(HNSPh2) belongs to the
monoclinic space group P2ð1Þ=c. There are two nearly
identical Cp*2UCl(OH)(HNSPh2) molecules and two
benzene molecules in the asymmetric unit leading to
eight molecules of Cp*2UCl(OH)(HNSPh2) and eight
benzene molecules in the unit cell. Least squares plane
calculations performed on the two benzene molecules in
the asymmetric unit with respect to the neighboring
phenyl groups indicate that these two benzenes are
symmetrically non-equivalent. The crystal, data collec-
tion and refinement information are summarized in
Table 1 and important bond lengths and bond angles
in Table 2. A perspective drawing of Cp*2UCl(OH)
(HNSPh2) is shown in Fig. 1.
2.2. Synthesis of Cp*2UCl(OH)(HNSPh2)
In a glove box, a solution of 73 mg (0.33 mmol) of
HNSPh2 ꢀ H2O in 10 ml of benzene was slowly added
to a solution of 193 mg (0.33 mmol) of Cp*2
UCl2(HNSPh2) in 15 ml of benzene. The sample turned
light green from dark orange and a white precipitate
began to form. After 3 h the solution was filtered
through a medium porosity frit and evaporated to dry-
ness. The green oily residue was dried under vacuum
overnight, dissolved in 3 ml of benzene and stored at
room temperature for a week during which period green
crystals formed. These crystals were separated from the
solution by filtration, rinsed with 2 ml of pentane and
dried under vacuum to yield 120 mg (63.7%) of
1
Cp*2UCl(OH)(HNSPh2). H NMR (d8-thf) at 23 °C:
)2.7 ppm (s, 30H, Cp*), )10.5 ppm (br), )0.5 (br), )163
ppm (br); at )60 °C: )4.1 ppm (Cp*, 30H), )2.0 ppm,
)0.5 ppm, )15.1 ppm, )163 ppm (br), 7.2 (br), 7.4 (br),
9.2 (br). IR (cmꢂ1): 3290 (w), 3150 (br), 3050 (s), 2900
(m), 2870 (m), 2250 (m), 1950 (s), 1875 (s), 1810 (s), 1560
(s), 1455 (m), 1440 (s), 1350 (w), 1250 (w), 1150 (m),
1075 (m), 1020 (w), 990 (w), 915 (w), 810 (m), 745 (s),
Table 1
Crystallographic data for Cp*2UCl(OH)(HNSPh2)
Identification code
Empirical formula
Formula weight
Hydp2
C38 H48 Cl N O S U
840.35
293(2)
Temperature (K)
Wavelength (A)
0.71073
Monoclinic, Pð2Þ1=c
Crystal system, space group
Unit cell dimensions
690 (s) cmꢂ1
.
Cp*2UCl(OH)(HNSPh2) decomposes in solution
over several days (Section 3) and more slowly at room
temperature in the solid phase. As a consequence of its
instability we were unable to obtain a satisfactory ele-
mental analysis.
ꢀ
a (A)
14.503(5)
30.095(11)
ꢀ
b (A)
ꢀ
c (A)
17.048(9)
90
a (°)
b (°)
c (°)
Volume
102.20(3)
90
7273(5) A3
8, 1.531
Z, Calculated density (Mg/m3)
2.3. Data collection and reduction of X-ray data
Absorption coefficient (mmꢂ1
)
4.623
3312
F (0 0 0)
Crystal size (mm)
Single crystals of Cp*2UCl(OH)(HNSPh2) were se-
lected, mounted and sealed in thin-walled glass capillaries
under dinitrogen. A Nicolet R3 computer-controlled
diffractometer with graphite-monochromated Mo Ka
1.0 ꢃ 0.5 ꢃ 0.5
1.59° to 22.56°
ꢂ15 6 h 6 15, ꢂ6 6 k 6 32,
ꢂ2 6 1 6 18
h Range for data collection
Limiting indices
ꢀ
ꢀ
Reflections collected/unique
Completeness to theta ¼ 22.56
Refinement method
10095/9343 ½RðintÞ ¼ 0:0511ꢄ
radiation (Ka1 ¼ 0:70930 A, Ka2 ¼ 0:71359 A) and a
scintillation detector with pulse height analyzer were used
for the measurement of diffraction intensities. During
data collection, the intensities of three standard reflec-
tions were re-measured every 97 reflections in the data
set. Data manipulation, structure solution and refine-
ment were carried out using SHELXL 97_2 Program
System [17]. Data were corrected for Lorentz and
97.5%
Full-matrix least-squares on F 2
9343/812/799
1.077
Data/restraints/parameters
Goodness-of-fit on F 2
Final R indices [I > 2rðIÞ]
R indices (all data)
Largest differential peak
and hole (e Aꢂ3
R1 ¼ 0:0651, wR2 ¼ 0:1630
R1 ¼ 0:0981, wR2 ¼ 0:1845
2.079 and )2.474
)