510
K.-T. Chen et al. / Inorganic Chemistry Communications 13 (2010) 506–510
at this temperature, the methyl and carbonyl carbons of OAcꢁ are
observed at 17.5 ppm [with 3J(Tl–C) = 200 Hz] and 174.7 ppm [with
2J(Tl–C) = 204 Hz] as doublets, respectively [11].
8.42 [o-H (22, 28)], 8.31 and 8.04 ppm for o0-H (34, 44) and o0-H
(38, 40) due to four different ortho protons of the aromatic ring
in 4 (Fig. 3b).
Due to the ring current effect, upfield shifts for the 1H reso-
nances of (o-Cl)BA-Ph-H6, (o-Cl)BA-Ph-H3, (o-Cl)BA-Ph-H5 and
X-ray diffraction analysis unambiguously confirms that 3 and 4
have a chelating bidentate OAcꢁ ligand in the solid state. The 13C
NMR chemical shifts were shown to be a useful tool for diagnosing
the nature of acetate ligands, whether unidentate or bidentate in
diamagnetic complexes. Unidentate acetate ligands were located
at 20.5 0.2 and 168.2 1.7 ppm and bidentate acetate ligands at
18.0 0.7 and 175.2 1.6 ppm [13]. The methyl and carbonyl
chemical shifts of the acetate group in 3 (or 4) at 20 °C in CDCl3
are separately located at 18.5 (or 18.9) and 175.0 (or 176.4) ppm
confirming that the acetate is chelating bidentately and is coordi-
nated to the thallium (or cadmium) atom in 3 (or 4) in the solution
phase.
In conclusion, we have investigated two new, diamagnetic and
mononuclear porphyrin complexes, namely, a thallium(III) com-
plex 3ꢀ0.5H2O and a cadmium(II) complex 4ꢀCH2Cl2 and their X-
ray structures are established. In 3, the N–H bond of the o-chloro-
benzamido ligand is cleaved and the o-chlorobenzamido nitrogen
participates in bonding to the thallium ion. Complex 3 is a bridged
metalloporphyrins with a metal–N–N linkage. In 4, the (o-Cl)BA
substituent is left intact and the cadmium(II) ion is coordinated
to the four nitrogens [N(1)–N(4)] of the macrocycle core. Com-
(o-Cl)BA-Ph-H4 for 4 in CDCl3 at 20 °C are
D
d = ꢁ3.2 [from 7.77
(obtained from o-chlorobenzamide) to 4.57 ppm], ꢁ1.46 (from
7.42 to 5.96 ppm), ꢁ1.34 (from 7.35 to 6.01 ppm) and ꢁ1.08
(from 7.40 to 6.32 ppm), respectively. As the distance between
the geometrical center (Ct) of the 4N plane [i.e., N(1), N(2), N(3),
N(4) for 3 and 4] and axial protons gets smaller, the shielding ef-
fect becomes larger. In 4, the distance for Ctꢀ ꢀ ꢀ(o-Cl)BA-Ph-H6,
Ctꢀ ꢀ ꢀ(o-Cl)BA-Ph-H3, Ctꢀ ꢀ ꢀ(o-Cl)BA-Ph-H5 and Ctꢀ ꢀ ꢀ(o-Cl)BA-Ph-H4,
increases from 5.419, 6.284, 7.057 to 7.396 Å. As the (o-Cl)BA-
Ph-H6 proton of 4 is closer to Ct, the shielding gets larger for this
(o-Cl)BA-Ph-H6 protons. A similar ring current effect is also ob-
served for 3. The average distance between Ctꢀ ꢀ ꢀ(o-Cl)BA-Ph-H6,
Ctꢀ ꢀ ꢀ(o-Cl)BA-Ph-H5, Ctꢀ ꢀ ꢀ(o-Cl)BA-Ph-H3 and Ctꢀ ꢀ ꢀ(o-Cl)BA-Ph-H4
for 3 increases from 3.233, 4.866, 5.946 to 5.984 Å. The 1H NMR
spectra reveal that the aromatic protons of the (o-Cl)BA group ap-
pear as a doublet of triplets at 6.36 ppm [(o-Cl)BA-Ph-H4], a dou-
blet at 6.21 ppm [(o-Cl)BA-Ph-H3], the triplet at 6.10 ppm [(o-
Cl)BA-Ph-H5] and the other doublet at 4.87 ppm [(o-Cl)BA-Ph-
H6] for 3. The (o-Cl)BA bonding argument is further supported
by the result that at 20 °C in 13C NMR the (o-Cl)BA-Ph-C1 [i.e.,
C(46)] and the C(45) peaks in 3 were observed at 132.6 ppm with
3J(Tl–C) = 20.1 Hz and at 167.7 ppm with 2J(Tl–C) = 665 Hz,
respectively.
pound
4 is a cadmium(II) N-substituted-N-aminoporphyrin
complex.
Acknowledgments
The 1H NMR spectrum for OAcꢁ of 4 in CD2Cl2 displays a sharp
The financial support from the National Research Council of the
ROC under Grant NSC 98-2113-M-005-005 is gratefully acknowl-
edged. We thank Dr. S. Elango for helpful discussions.
singlet for CH3 at d0.06 ppm with
a sharp singlet for the same methyl proton at d ꢁ0.01 ppm with
1/2 = 4 Hz at ꢁ90 °C. This minimum deviation in the value of line
width (
1/2) upon cooling indicates that OAcꢁ exchange does not
Dm1/2 = 3 Hz at 20 °C and remains
D
m
D
m
occur in compound 4.
Appendix A. Supplementary material
Upon cooling of a 0.02 M CD2Cl2 solution of 3, the methyl pro-
ton signal of OAcꢁ, being a single peak at 20 °C (d 0.17 ppm), first
broadened (coalescence temperature Tc = ꢁ75 °C) and then split
into peaks with a separation of 14.4 Hz at d 0.08 ppm at ꢁ90 °C.
As the exchange of OAcꢁ within 3 is reversible, the results at
599.95 MHz confirm the separation as a coupling of 4J(Tl–H) rather
than a chemical shift difference [10,11]. The most likely cause of
loss of coupling is due to the reversible dissociation of acetate with
a small dissociation constant.
CCDC 695921 (for 3ꢀ0.5H2O) and 695922 (4ꢀCH2Cl2) contain the
supplementary crystallographic data for this paper. These data can
be obtained free of charge from The Cambridge Crystallographic
tary data associated with this article can be found, in the online
References
TlðN-NCOðo-ClÞC6H4-tppÞðOAcÞ
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CD2Cl2
*
)
TlðN-NCOðo-ClÞC6H4-tppÞþ þ OAcꢁ
ð1Þ
Such a scenario would lead to the change in the chemical shift with
temperature and no detectable free OAcꢁ and Tl(N-NCO(o-Cl)C6H4-
tpp)+ at low temperature, but would lead to the loss of coupling be-
tween acetate and thallium at higher temperature [10–12]. The
chemical shift in the high-temperature limit is the average of the
two species (i.e., Tl(N-NCO(o-Cl)C6H4-tpp)(OAc) and OAcꢁ) in Eq.
(1) weighted by their concentration. The free energy of activation
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at the coalescence temperature Tc for the intermolecular exchange
–
of OAcꢁ in 3 is determined to be
D
G198 ¼ 42:1 kJ/mol. At 20 °C,
intermolecular exchange of the OAcꢁ group for 3 is rapid as indi-
cated by the appearance of singlet signals due to carbonyl carbons
at 175.0 ppm and methyl carbons at 18.5 ppm. At ꢁ90 °C, the rate
of intermolecular exchange of OAcꢁ for 3 in CD2Cl2 is slow. Hence,
[13] S.J. Lin, T.N. Hong, J.Y. Tung, J.H. Chen, Inorg. Chem. 36 (1997) 3886.