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N. Xu et al. / Inorganica Chimica Acta 469 (2018) 183–188
10 min before each set of measurements, and then the nitrogen
atmosphere was maintained during the measurements which were
performed at room temperature (ꢀ20 °C). Scan rates of 200–
1000 mV/s were used, but no significant differences in the cyclic
voltammogram profiles were noted.
Infrared spectra for the synthetic work were collected on a Bio–
Rad FT–155 FTIR spectrometer. For infrared spectroelectrochem-
istry, the experimental setup consisted on the same cell utilized
for the cyclic voltammetry measurements, with the 3 mm Pt disk
working electrode serving as the mirror for the fiber optic mid-IR
dip probe, as described previously [14–16]. The resulting IR spectra
refinement. The structure was solved by direct methods and
refined by full-matrix least-squares methods on F2 [22,23]. Hydro-
gen atom positions were initially determined by geometry and
refined using a riding model. Non-hydrogen atoms were refined
with anisotropic displacement parameters. Hydrogen atom dis-
placement parameters were set to 1.2 times the displacement
parameters of the bonded atoms. A total of 505 parameters were
refined against 9144 data to give wR(F2) = 0.1638 and S = 1.012
for weights of w = 1/[
[F2o + 2F2c]/3. The final R(F) was 0.0655 for the 5690 observed,
[F > 4 (F)], data.
r
2(F2) + (0.0680 P)2 + 1.9000 P], where P =
r
were recorded using
a
Bruker Vector 22 FTIR spectrometer
The largest shift/s.u. was 0.003 in the final refinement cycle. The
final difference map had maxima and minima of 0.616 and
ꢂ0.876 e/Å3, respectively. Displacement ellipsoids in Fig. 1 are
drawn at the 35% probability level. Details of the crystal data and
refinement are given in Table 1. CCDC 1444107 contains the crys-
tallographic data for this paper. These data can be obtained free of
ing deposit@ccdc.cam.ac.uk, or by contacting The Cambridge Crys-
tallographic Data Centre, 12, Union Road, Cambridge CB2 1EZ, UK;
fax: +44 1223-336-033
equipped with a liquid nitrogen cooled MCT detector (Remspec
Corporation, Sturbridge, MA, USA). UV–Vis spectra were recorded
on a Hewlett-Packard model 8453 diode array instrument.
2.4. Synthesis
Three iron porphyrin acetate compounds were prepared in a
manner similar to that used for the preparation of (por)Fe(OC
(=O)R) analogues [17]. The following is representative:
(TPP)Fe(OC(=O)CCl3 (1). To a CH2Cl2 solution (15 mL) of [(TPP)
Fe]2(l-O) (0.033 g, 0.024 mmol) was added trichloroacetic acid
(0.010 g, 0.06 mmol). The mixture was stirred for 45 min, during
which time the color of the solution changed from green to brown.
The solvent was reduced to ꢀ3 mL and hexane (10 mL) was added.
The solution was slowly concentrated under reduced pressure until
precipitation of the product occurred. The dark brown precipitate
was collected by filtration, washed with hexane (2 ꢁ 15 mL), and
dried in vacuo to give (TPP)Fe(OC(=O)CCl3) (0.020 g, 0.024 mmol,
50% isolated yield). Slow evaporation of a CH2Cl2/cyclohexane
(1:1 ratio; 4 mL) solution of the product at room temperature gave
suitable crystals for X-ray diffraction studies. IR (CH2Cl2, cmꢂ1):
t
OCO(asym) = 1704. IR (KBr, cmꢂ1):
tOCO(asym) = 1709. UV–vis (k
(relative
(14), 571 (8), 681 (4) nm.
e
, mMꢂ1cmꢂ1), 2 ꢁ 10ꢂ5 M in CH2Cl2): 411 (138), 509
The other iron acetate porphyrin complexes were generated
similarly using the respective porphyrin and acid precursors.
(TPP)Fe(OC(=O)CH2Cl) (2). Isolated yield: 60%. IR (CH2Cl2,
cmꢂ1):
UV–vis (k (relative
(36), 412 (109), 507 (8), 573 (9), 656 (7) nm.
t tOCO(asym) = 1692.
OCO(asym) = 1684. IR (KBr, cmꢂ1):
e
, mMꢂ1cmꢂ1), 1 ꢁ 10ꢂ5 M in CH2Cl2): 351
(OEP)Fe(OC(=O)CCl3) (3) [18]. Isolated yield: 65%. IR (CH2Cl2,
cmꢂ1):
UV–vis (k (relative
(98), 506 (7), 533 (7), 634 (3) nm.
t tOCO(asym) = 1711.
OCO(asym) = 1704. IR (KBr, cmꢂ1):
e
, mMꢂ1cmꢂ1), 8 ꢁ 10ꢂ6 M in CH2Cl2): 381
2.5. X-ray crystallography
A black plate-shaped crystal of (TPP)Fe(OC(=O)CCl3) (1) of
dimensions 0.28 ꢁ 0.26 ꢁ 0.05 mm was selected for structural
analysis. Intensity data for this compound were collected using a
diffractometer with a Bruker APEX ccd area detector [19,20] and
graphite-monochromated Mo K
a radiation (k = 0.71073 Å). The
sample was cooled to 100(2) K. Cell parameters were determined
from a non-linear least squares fit of 8508 peaks in the range
2.21 < h < 27.37°. A total of 62935 data were measured in the range
1.689 < h < 28.456° using / and
x oscillation frames. The data were
corrected for absorption by the semi-empirical method [21] giving
minimum and maximum transmission factors of 0.833 and 0.967.
The data were merged to form a set of 9144 independent data with
R(int) = 0.1583 and a coverage of 100.0%.
The monoclinic space group P21/n was determined by system-
atic absences and statistical tests and verified by subsequent
Fig. 1. (a) Molecular structure of (TPP)Fe(OC(=O)CCl3) (1). Hydrogen atoms are
omitted for clarity, and thermal ellipsoids are drawn at the 35% probability level. (b)
Perpendicular displacements (in units of 0.01 Å) of the porphyrin core atoms from
the 24-atom mean porphyrin plane. Selected bond lengths (in Å) and angles (in
deg): Fe–N1 = 2.044(3), Fe–N2 = 2.046(3), Fe–N3 = 2.046(3), Fe–N4 = 2.054(3), Fe–
O1 = 1.917(2), \Fe–O1–C45 = 133.2(2).