Angewandte
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for 2a,b. Comparison with authentic samples showed that the
latter corresponded to remaining traces of the free diolamide
ligands of 1a, 2a,b that did not get anchored to the POM
scaffold. In both the free diolamides and the organo-POMs,
the proton resonances of the amide in the pyridine derivatives
are from 1 to 1.5 ppm downfield compared to their analogous
1
benzamide derivative. In the H-15N HSQC experiments one
can only observe the 15N resonance of atoms that are directly
bound to a proton. Thus there is no cross peak corresponding
to the pyridine nitrogen of 2a and 2b. The 15N resonances shift
from about 120 ppm in the free ligands to about 160 ppm in
the organo-POMs and they do not vary much in the different
POMs. Simultaneously, the 1H signals are also strongly shifted
downfield (2 ppm average shift) in the organo-POMs, as
mentioned above.
=
Figure 2. TBA5[P2V3W15O59{(OCH2)2C(Et)NHC( O@POM)R}] organo-
POMs considered in this work.
influence the acidity. POM 1d was prepared in 99% yield
using our established method. We also prepared pyridine
derivatives 2a,b,[5c] which have an internal basic site.
The most noticeable feature of POMs 1a–d is the
chemical shift of the proton of the grafted amide in CD3CN.
It ranges from 9.15 ppm for 1c to 9.86 ppm for 1b, with POM
1a at 9.32 ppm and 1d at 9.68 ppm. The chemical shift for 2a
and 2b is 10.40 ppm. This suggests that the iminium resonance
form of the amide might be stabilized by the POM structure.
However, it might also be possible that the amide would be
deprotonated, and the proton released would remain on the
POM as a counterion. To discriminate between these two
options, we decided to monitor the amide resonance with 2D
1H-15N HSQC experiments at natural nitrogen isotopic
abundance (see Supporting Information for details) on
POMs 1a, 2a,b.
The observation of crosspeaks demonstrates that the
target proton remains bound to the amide in the POMs, as
1
does the significant H chemical shift difference between 1a
and 2a,b. The latter certainly reflects the different magnetic
environment of the amide when substituted by a phenyl ring,
relative to an electronically different pyridine ring. This
difference would likely be less pronounced if the protons were
attached to the metal oxide surface, far from the substituents.
1
The strong downfield shift observed in H and 15N supports
our assumption that upon coordination of the amide oxygen
to the vanadate atoms the amide assumes a higher imidate
character (Figure 1, top right) with a partial positive charge
on the nitrogen that is likely responsible for the downfield
shifts.
In order to further validate our hypothesis, we performed
DFT calculations at the BP86/LANL2DZ level of theory
within the Gaussian09 suite of programs[6] for the protonated
and deprotonated hybrid-POM molecules. An implicit sol-
vent correction was added to model the acetonitrile. The
example of 1a is shown in Figure 4. In the protonated form
Figure 3 shows the overlap of the HSQC spectra acquired
on the POMs. Strong cross-peaks were observed for the amide
with a 15N chemical shift of about 160 ppm and H chemical
1
shifts ranging from 9.4 for 1a to 10.4 ppm for 2a and 2b. In
the same spectrum, we also observed weak cross-peaks at
around 120 ppm for nitrogen and 6.9 ppm for 1a, 8.6–8.7 ppm
=
(upper panel, a), the HN-C(Ph) O bond length was calcu-
=
lated at 1.36 , and that of the C O bond was 1.28 . The
=
phenyl group appears slanted and the V-O( C)-V bridge is
À
À
distorted, with the V O bond facing the C H of the phenyl
À
longer than the V O bond on the other side (2.26 vs.
À
2.35 ). The N C bond connecting the amide group to the
diol part is 1.51 long. In the deprotonated form (lower
=
panel, b), the N-C(Ph) O bond length shortens to 1.31 ,
=
while the C O bond is lengthened (1.37 ). The phenyl group
=
is much less slanted, and the V-O( C)-V bridge is sym-
À
À
metrical (equal V O bond lengths at 2.13 ). The N C bond
connecting the amide group to the diol part is unchanged
(1.50 ). This trend is similar for all the systems calculated,
including the pyridine derivatives (Table S1 and Fig-
ures S1,S2).
1
We then computed the H NMR chemical shifts of the
amide proton of all POMs studied (in their N-protonated
forms), using the GIAO protocol, at the PBE1PBE/
LANL2DZ//BP86/ LANL2DZ level of theory. The calculated
values were in very good linear agreement with the observed
shifts (Figure S3, R2 = 0.952), with a systematic deviation of
0.33 ppm. Finally, we calculated the proton affinities for 1a.
This was carried out to explore the possibility of a protonation
on the oxo ligands of the POM structure. The proton affinity
Figure 3. Superposition of the 1H-15N HSQC spectra of the hybrid-
POM solution in CD3CN (1a: 5 mm, 2a: 2.3 mm, 2b: 7.5 mm;
T=298 K). The spectra were acquired at 14.1 T (600 and 60.8 MHz for
1H and 15N respectively) using 512128 complex points with 64 scans,
4.0 s of recycle delay, and FID acquisition times of 17.5 ms and
53.2 ms in the indirect and direct dimension, respectively. The 2D FID
was processed with a 1024512 complex matrix points with square-
cosine windows functions for both the direct and indirect dimensions.
ꢀ 2016 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2016, 55, 5961 –5965