Communications
room temperature. As the temperature increases, the inten-
sity of these bands decreases (Figures S7 and S8, Supporting
Information). At 433 K, these bands almost disappear, that is,
all H O molecules are removed from 2. On the other hand,
2
bands due to the DODA cation and the POM ring scarcely
change. The UV spectra of 2 before and after removal of all
H O in CHCl solution are similar to each other (Figure S9,
2
3
Supporting Information). These results suggest that removal
of all H O molecules has little influence on the ring structure
2
of 2. The irregular assembly of the ring-shaped POMs, as
shown in Scheme 1, was confirmed by XRD patterns, in which
only some of the broad peaks of 2 were identifiable
(
Figure S10, Supporting Information), and this gives a very
Figure 1. Adsorption isotherms of N and CO in dehydrated 1 (N :
interesting perspective for future design of these architec-
tures, since a regular assembly of POMs with designed (e.g.,
rigid) cations has potential to give access to a more prominent
nanospace.
2
2
2
circles, CO : squares) and 2 (N : triangles, CO : diamonds) at 77 and
2
2
2
195 K (adsorption: empty symbols, desorption: filled symbols).
In the case of hybrid 2, it is important whether the DODA
cations are located inside or outside the {Mo154} ring. The
1
[9]
H NMR spectra of 2 in CDCl3 indicate that the electrostatic
interaction between the negatively charged {Mo154} ring and
positively charged nitrogen atom of DODA reduces the
motional freedom of the head group of the DODA cation,
and the relatively large thermal motions of the two octadecyl
chains of DODA cations are maintained. In addition, the
observation that 2 is highly soluble in nonpolar solvents such
as toluene, CH Cl , and CHCl , as well as the fact that the
2
2
3
DODA cation is considerably larger than the inner space of
the wheel, indicates that the DODA cations are predom-
inately located on the outside of the {Mo154} ring. Further-
more, the maximum adsorbed amount of H O molecules also
2
supports our suggestion. This idea can be expanded further by
considering that the inner volume of the {Mo154} ring
Figure 2. Adsorption isotherms of H O (circles), MeCN (squares), and
benzene (triangles) in dehydrated 2 at 298 K (adsorption: empty
2
calculated from the inner diameter and the height is about
symbols, desorption: filled symbols).
3
4
.1 nm , while up to 150H O molecules can be adsorbed per
2
{
Mo154} ring. Considering the liquid density of H O, the
2
3
adsorbed H O molecules occupy a volume of about 4.5 nm ,
All isotherms for dehydrated 2 show a gradual increase in the
amount of gas adsorbed. In addition, the higher the mea-
surement temperature is, the more the adsorbed amount
increases. These results support that the gases and vapors
diffuse into densely aggregated alkyl chains of DODA cations
with structural transformations, that is, positional displace-
2
which is similar to the inner volume of the {Mo154} ring.
Further, the amount of H O adsorbed by 2 is significantly
2
lower than the amount in as-synthesized 1 (ca. 470). In the
case of as-synthesized 1, a large amount of H O is located on
2
the outside of the {Mo154} ring, while the outer space of 2 is
occupied by alkyl chains of DODA cations, which decrease
ments of alkyl chains. The fact that the hydrophilic H O,
2
the amount of H O adsorbed by 2. Considering the high
hydrophobic benzene, and medium-polarity MeCN are all
adsorbed by dehydrated 2 indicates coexistence of a hydro-
philic nanospace formed inside the {Mo154} ring and hydro-
phobic nanospace existing inside the aggregated alkyl chains.
Infrared spectra of pyridine-loaded 2 (Figure 3) were
measured to explore the presence of Lewis and Brønsted
acidic sites inside the {Mo154} ring. The positions of in-plane
vibration bands of a pyridine ring strongly depend on its
2
hydrophilicity of H O, it can be concluded that the inner space
2
is largely filled with H O molecules, and the outer surface is
2
covered by the DODA cations.
To confirm the presence of the nanospace after removal of
all H O molecules, gas and vapor adsorption isotherms were
2
measured on samples that had been dried at 353 K under
vacuum. Figure 1 shows the adsorption isotherms of N and
2
[12]
À1
CO at 77 and 195 K. Dehydrated “unprotected” 1 shows no
binding state.
The bands at 1539 and 1456 cm are
2
adsorption of N and CO over the entire pressure range, and
attributed to pyridine adsorbed on Brønsted and Lewis
acidic site, respectively, and a band at 1442 cm , derived
2
2
À1
this indicates that dehydrated 1 has no accessible space for
these gases. In contrast, the adsorption isotherms of desol-
vated “protected” 2 show gradual uptake, that is, dehydrated
from hydrogen-bonded pyridine, is also observed. Because of
the high affinity for H O molecules, H O molecules are easily
2
2
2
has a permanent and accessible nanospace. The adsorption
adsorbed by 2 during the handling of dehydrated 2 in the
atmosphere, which was confirmed by TG and IR measure-
ments (see Figures S6 and S11, Supporting Information).
isotherms of H O, MeCN, and benzene for dehydrated 2 at
2
2
98 K (Figure 2) also show gradual uptake by the nanospace.
ꢀ 2009 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2009, 48, 8703 –8706