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C.-G. Yan et al. / Journal of Organometallic Chemistry 585 (1999) 63–67
mmol) of triethylamine and 0.21 ml (2.00 mmol) ben-
zeneselenol. The mixture was stirred at r.t. for 30 min
and the solution turned to red–brown. The resulting
[Et3NH][(m-PhSe)(m-CO)Fe2(CO)6] (1) reagent solution
was cooled to 0°C and added by cannula 0.65 g (3.00
mmol) N-phenylbenzimidoyl chloride dissolved in a
separate flask in 15 ml THF. The mixture was stirred at
r.t. for 24 h. The solvent was removed under vacuum to
leave a red residue, which was extracted with petroleum
ether and purified by filtration chromatography, then
purified further by TLC using petroleum ether as elu-
ent. The first red band gave 0.271 g (23%) of (m-
PhSe)2Fe2(CO)6, which was identified by comparison of
its melting point and 1H-NMR spectrum with those
given in the literature [5]. The second red band gave
0.347 g (28%) of (m-PhSe)(s,m-PhCꢀNPh)Fe2(CO)6 (3c)
as a red solid. M.p. (dec.) 140–141°C. Anal. Calc. for
C25H15Fe2NO6Se: C, 48.74; H, 2.45. Found: C, 48.44;
H, 2.76%. 1H-NMR (CDCl3): l 6.55–7.70 (3 C6H5)
ppm. IR (KBr, disc): w 2069(s), 2021(vs), 1991(vs),
3.7. Crystal structure determination of 3c
A red prismatic crystal of C25H15O6NSeFe2 having
approximate dimensions of 0.20×0.20×0.30 mm was
mounted on a glass fiber. All measurements were made
on a Rigaku AFC7R diffractometer with graphite
monochromated Mo–Ka radiation and a 12 kW rotat-
ing anode generator. Cell constants and an orientation
matrix for data collection, obtained from a least-
squares refinement using the setting angles of 18
carefully centered reflections in the range 18.333°B
2qB24.42° corresponded to a primitive triclinic cell.
The data were collected at a temperature of 2091°C
using the ꢀ−2q scan technique to a maximum 2q
value of 50.0°. ꢀ scans of several intense reflections,
made prior to data collection, had an average width at
half-height of 0.10 with a take-off angle of 6.0°. Scans
of (1.21+0.30 tan q) were made at a speed of 16.0
min−1 (in ꢀ). The weak reflections [IB13.0|(I)] were
rescanned (maximum of four scans) and the counts
were accumulated to ensure good counting statistics.
Stationary background counts were recorded on each
side of the reflection. The ratio of peak counting time
to background counting time was 2:1. The diameter of
the incident beam collimator was 1.0 mm, the crystal to
detector distance was 235 mm, and the computer con-
trolled detector aperture was to 9.0×13.0 mm (hori-
zontal×vertical). Of the 3641 reflections that were
collected, 3392 were unique [Rint=0.018]. The intensi-
ties of three representative reflection were measured
after every 200 reflections. Over the course of data
collection, the standards decreased by −1.1%. A linear
correction factor was applied to the data to account for
this phenomenon. The linear absorption coefficient v
for Mo–Ka radiation is 26.6 cm−1. An empirical ab-
sorption correction based on azimuthal scans of several
reflections was applied which resulted in transmission
factors ranging from 0.58 to 1.00. The data were cor-
rected for Lorentz and polarization effects. A correc-
tion for secondary extinction was applied where the
coefficient=2.433296e-06.
1975(vs), 1950(s) (CꢁO), 1530(m) (CꢀN) cm−1
.
3.5. Reaction of [Et3NH][(v-PhSe)(v-CO)Fe2(CO)6] (1)
with Ph(Cl)CꢀNC6H5CH3-p
The same procedure as for 3c was followed, but 0.690
g (3.00 mmol) of Ph(Cl)CꢀNC6H4CH3-p was used in-
stead of Ph(Cl)CꢀNPh. The first red band gave 0.209 g
(18%) of (m-PhSe)2Fe2(CO)6, which was identified by
comparison of its melting point and 1H-NMR spectrum
with those given in the literature [5]. The second red
band gave 0.350
PhCꢀNC6H4CH3-p)Fe2(CO)6 (3d) as a red solid. M.p.
(dec.) 142–144°C. Anal. Calc. for C26H17Fe2NO6Se: C,
g
(28%) of (m-PhSe)(s,m-
1
49.56; H, 2.72. Found: C, 50.02; H, 3.04%. H-NMR
(CDCl3): l 2.13 (s, 3H, CH3), 6.74, 7.38 (d, d, J=7.0
Hz, 2H, 2H, C6H4), 6.89–7.37 (2 C6H5) ppm. IR (KBr,
disc): w 2069(vs), 2020(vs), 1991(vs), 1975(vs), 1944(s)
(CꢁO), 1535(m) (CꢀN) cm−1
.
3.6. Reaction of [Et3NH][(v-PhSe)(v-CO)Fe2(CO)6] (1)
with Ph(Cl)CꢀNC6H5Cl-p
The structure was solved by direct methods and
expanded using Fourier techniques. The non-hydrogen
atoms were refined anisotropically. Hydrogen atoms
were refined isotropically. The final cycle of full-matrix
least-squares refinement was based on 2688 observed
reflections [I\3.00|(I)] and 377 variable parameters
and converged (largest parameter was 0.04 times its
estimated S.D.) with unweighted and weighted agree-
ment factors of R=0.026, Rw=0.033. The standard
deviation of an observation of unit weight [Sw(ꢀFoꢀ−
ꢀFcꢀ)/(No−Nv)]1/2=1.29 (No=number of observations,
Nv=number of variables). The weighting scheme was
based on counting statistics and included a factor (p=
0.030) to downweight the intense reflections. Plots of
Sw(ꢀFoꢀ−ꢀFcꢀ) versus ꢀFoꢀ, reflection order in data col-
The same procedure as for 3c was followed, but 0.615
g (3.00 mmol) of Ph(Cl)CꢀNC6H4Cl-p was used instead
of Ph(Cl)CꢀNPh. The first red band gave 0.313 g (26%)
of (m-PhSe)2Fe2(CO)6, which was identified by compari-
1
son of its melting point and H-NMR spectrum with
those given in the literature. The second red band gave
0.514
g
(40%) of (m-PhSe)(s,m-PhCꢀNC6H4Cl-
p)Fe2(CO)6 (3e) as a red solid. M.p. (dec.) 124–126°C.
Anal. Calc. for C25H15ClFe2NO6S: C, 46.16; H, 2.17.
1
Found: C, 46.35; H, 2.56%. H-NMR (CDCl3): l 6.53–
7.53 (2 C6H5, C6H4) ppm. IR (KBr, disc): w 2067(vs),
2020(vs), 1992(vs), 1978(vs), 1945(s) (CꢁO), 1540(m)
(CꢀN) cm−1
.