12102 J. Am. Chem. Soc., Vol. 121, No. 51, 1999
Wang et al.
oscillation range of 2°/frame and an exposure time of 60 s/deg.88
oxime: 1H NMR (C6D6, 2mM, 25 °C, 500 MHz) δ 6.80 (t, J ) 7.5
Hz, 1H, 2-fluorenoneoximyl H), 6.93 (t, J ) 7.5 Hz, 1H, 7-fluorenone-
oximyl H), 6.95 (t, J ) 7.5 Hz, 1H, 3-fluorenoneoximyl H), 6.97 (t, J
) 7.5 Hz, 2H, 2-fluorenyl H), 7.01 (t, J ) 7.5 Hz, 1H, 6-fluorenone-
oximyl H), 7.06 (t, J ) 7.5 Hz, 1H, 3-fluorenyl H), 7.11 (d, J ) 7.5
Hz, 1H, 4-fluorenoneoximyl H), 7.12 (d, J ) 7.5 Hz, 1H, 5-fluorenone-
oximyl H), 7.20 (d, J ) 7.5 Hz, 2H, 4-fluorenyl H), 7.64 (d, J ) 7.5
Hz, 1H, 8-fluorenoneoximyl H), 8.02 (d, J ) 7.5 Hz, 2H, 1-fluorenyl
H), 8.30 (d, J ) 7.5 Hz, 1H, 1-fluorenoneoximyl H); IR (CDCl3) νNO2
1561 (vs), 1349 (s); νNO 989 (vs); νCO 1036 cm-1 (s).
X-ray Crystallography. General Procedure. X-ray crystallographic
studies were carried out on a Nonius KappaCCD diffractometer
equipped with graphite-monochromatized Mo KR radiation (λ )
0.710 73 Å). Samples were either mounted on a glass fiber with epoxy
cement or sealed in a glass capillary, and the diffraction data were
collected at room temperature. Relevant crystallographic information
is listed in Table 1.
A
total of 79 647 reflections (θmax ) 27.46°) were indexed, integrated,
and corrected for Lorentz and polarization effects using DENZO-SMN
and SCALEPACK.89 Data reduction yielded 13 775 unique reflections
(Rint ) 0.0490) of which 7272 had I > 2σ(I). Postrefinement of the
unit cell parameters gave a ) 12.5029(2) Å, b ) 13.0424(4) Å, c )
18.9793(5) Å, R ) 81.701(1)°, â ) 88.304(2)°, γ ) 84.263(2)°, and
V ) 3046.80(13) Å3. Axial photographs and a lack of systematic
absences suggested that the compound had crystallized in the triclinic
space group P1 or P1h. The latter space group P1h (No. 2) was selected
on the basis of an observed mean value of 0.901 for |E* E - 1| (versus
the expectation values of 0.968 and 0.736 for centric and noncentric
data, respectively).
The structure was solved by direct methods and refined by full-
matrix least squares on F2 using SHELXTL90 to R(F) ) 0.1545 and
wR(F2) ) 0.3066 for 13 775 unique reflections. A disordered chlo-
robenzene solvent molecule was included in the refinement, and two
additional carbon atoms were placed at a second (presumably heptane)
solvent site. The chlorobenzene did not refine well, and the identity of
the second solvent molecule could not be assigned via a discrete-atom
approach. Therefore, the analysis was resumed with the following
solvent-free model.
X-ray Crystal Structure Determination of O-(9-Nitro-9-fluore-
nyl)fluorenone Oxime (1). Single crystals of 1 suitable for X-ray
crystallographic analysis were obtained by slow diffusion of CH3CN
into a benzene solution of 1 over a period of 1 week. A pale yellow
irregular chunk (0.15 mm × 0.20 mm × 0.25 mm in size) was used
for the diffraction experiment (Table 1). A total of 608 frames of data
were collected at 298(2) K with an oscillation range of 1°/frame and
The SQUEEZE/BYPASS procedure93 implemented in PLATON94
was used to account for the solvent electron density. Two solvent-
accessible voids were detected. The first of these two voids is situated
along the crystallographic c-axis (0, 0, z) and has a volume and electron
count of 482 Å3 and 92 e, respectively. From our discrete-atom approach
mentioned above, we know that this void is occupied by two
chlorobenzene molecules (339 Å3, 116 e). The second void is situated
at the center of the cell (0.5, 0.5, 0.5) and has a volume and electron
count of 245 Å3 and 55 e, respectively. These results suggest that the
occupant of this second void may be a molecule of the precipitating
solvent heptane (244 Å3, 58 e) used in recrystallizing the iron complex.
Since there are two molecules of the iron complex per cell, the chemical
formulation C57H28Cl8FeN5O‚6H5Cl‚.5C7H16 is proposed.
an exposure time of 120 s/deg.88 A total of 26 402 reflections (θmax
22.48°) were indexed, integrated, and corrected for Lorentz and
polarization effects using DENZO-SMN and SCALEPACK.89 The θmax
limit was reduced from the standard 27.50° due to the sample being a
)
poor scatterer. Data reduction yielded 2622 unique reflections (Rint
)
0.0530) of which 1948 had I > 2σ(I). Postrefinement of the unit cell
parameters gave a ) 9.8776(6) Å, b ) 11.9206(6) Å, c ) 17.4262-
(12) Å, â ) 101.550(3)°, and V ) 2010.3(2) Å3. Axial photographs
and systematic absences were consistent with the compound having
crystallized in the monoclinic space group P21/n (No. 14).
The structure was solved by direct methods and refined by full-
matrix least squares on F2 using SHELXTL.90 All of the non-hydrogen
atoms were refined with anisotropic displacement coefficients. The
hydrogen atoms were assigned isotropic displacement coefficients U(H)
) 1.2U(C), and their coordinates were allowed to ride on their
respective carbons. Nearly 50% of the structure was found to be
disordered. The disorder was treated with a two-site model as follows:
[O(1), N(1), C(1), C(2), C(3), C(4), C(4A), C(4B), C(5), C(6), C(7),
C(8), C(8A), C(9), C(9A)] and [O(1*), N(1*), C(1*), C(2*), C(3*),
C(4*), C(4A*), C(4B*), C(5*), C(6*), C(7*), C(8*), C(8A*), C(9*),
C(9A*)]. The partial atoms at these two sites were assigned occupancy
factors of a half and the carbons refined with mild distance restraints.
The SQUEEZE-processed data were used in all subsequent cycles
of least squares. All of the nonhydrogen atoms were refined with
anisotropic displacement coefficients. The hydrogen atoms were
assigned isotropic displacement coefficients U(H) ) 1.2U(C), and their
coordinates were allowed to ride on their respective carbons. The
weighting scheme employed was w ) 1/[σ2(Fo ) + (0.0838P)2], where
2
2
P ) (Fo + 2Fc2)/3. The refinement converged to R(F) ) 0.0571,
wR(F2) ) 0.1490, and S ) 1.32 for 7272 reflections with I > 2σ(I),
and R(F) ) 0.1155, wR(F2) ) 0.1681, and S ) 1.07 for 13 775 unique
reflections and 649 parameters. The maximum ∆/σ in the final cycle
of least squares was less than 0.001, and the residual peaks on the
final difference Fourier map ranged from -0.298 to 0.443 eÅ-3
.
The weighting scheme employed was w ) 1/[σ2(Fo ) + (0.0551P)2 +
2
0.7277P], where P ) (Fo2 + 2Fc2)/3. The refinement converged to R(F)
) 0.0569, wR(F2) ) 0.1407, and S ) 1.20 for 1948 reflections with I
> 2σ(I), and R(F) ) 0.0772, wR(F2) ) 0.1529, and S ) 1.09 for 2622
unique reflections, 416 parameters, and 72 restraints. The maximum
∆/σ in the final cycle of leas -squares was less than 0.001, and the
residual peaks on the final difference Fourier map ranged from -0.094
to 0.160 eÅ-3. Scattering factors were taken from the International
Tables for Crystallography, Volume C.91,92
Scattering factors were taken from the International Tables for
Crystallography, Volume C.91,92
Titration of Fe(OH)TMP with Fluorenone Oxime. To 0.8 mL of
a benzene-d6 solution of Fe(OH)TMP (2.4 mM) was added small
aliquots of solid fluorenone oxime. A 1H NMR spectrum of the sample
was taken after thorough mixing. The spectrum showed that the
resonance signals of Fe(OH)TMP changed to those of 2 within minutes,
and the amount of 2 generated was proportional to that of the oxime
added. The conversion was complete upon the addition of 1 equiv of
fluorenone oxime. Further addition of fluorenone oxime led to the
emergence of the signals of free fluorenone oxime without interfering
signals of any other species.
Oxidation of Fe(oximate)TMP (2) at High O2 Pressures. A high-
pressure reaction vessel was made from stainless steel by our
departmental machine workshop. The reactor contains a 30 mL Teflon
liner, and the high-pressure seal was achieved by pressing an O-ring
between the stainless steel screw-cap and the Teflon liner. The pressure
gauge on top of the reactor monitoring the presure in the liner and two
separate gas inlet and outlet values allow the control of the gas content
inside the Teflon liner.
X-ray Crystal Structure Determination of Fe(oximate)TDCPP
(3). Single crystals of 3 suitable for X-ray crystallographic analysis
were obtained by slow diffusion of n-heptane into a chlorobenzene
solution of 3 over 3 days. A dark purple prism cut to 0.12 mm × 0.28
mm × 0.35 mm in size was used for the diffraction experiment (Table
1). A total of 493 frames of data were collected at 298(2) K with an
(88) COLLECT Data Collection Software. Nonius B. V. Rontgenweg 1
P.O. Box 811, 2600 AV, Delft, The Netherlands, 1998.
(89) Otwinowski, Z.; Minor, W. Methods Enzymol. 1997, 276, 307.
(90) Sheldrick, G. M. SHELXTL Version 5.04.; Siemens Analytical X-ray
Instruments: Madison, WI, 1996.
(91) Maslen, E. N.; Fox, A. G.; O’Keefe, M. A. In International Tables
for Crystallography: Mathematical, Physical and Chemical Tables; Wilson,
A. J. C., Ed: Kluwer: Dordrecht, The Netherlands, 1992; Vol. C, p 476.
(92) Creagh, D. C.; McAuley, W. J. In International Tables for
Crystallography: Mathematical, Physical and Chemical Tables; Wilson,
A. J. C., Ed: Kluwer: Dordrecht, The Netherlands, 1992; Vol. C, p 206.
A 2 mL silanized glass vial containing a 0.8 mL benzene-d6 solution
of 0.75 mM 2 was enclosed in the high-pressure reactor. The reaction
(93) Van der Sluis, P.; Spek, A. L. Acta Crystallogr., A 1990, 46, 194.
(94) Spek, A. L. Acta Crystallogr., A 1990, 46, C34.