A Tripodal Host with Cylindrical Conformation
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ture, and the distinct form IV with open channels is ob-
tained in some situations. Therefore, solvatomorphism of
host molecules largely depends on the intrinsic properties of
guest molecules, such as size, shape, and self-interaction,
and these conclusions give new insight into the inclusion be-
havior of the tripodal host molecules.
mained (Figure S5 in the Supporting Information). Unfortu-
nately, resultant opaque material 4x is devoid of single crys-
tallinity, so the use of single-crystal X-ray diffraction for
structural identification is precluded. This solid–solid phase
transformation of molecular material is very interesting be-
cause it may form an active phase that rapidly adsorbs gases
under ambient conditions, especially for a synthetic host
with a permanent cavity.[4a,21] Further investigation into the
structure and application in gas adsorption of 4x are under-
way.
Thermogravimetric analysis (TGA): The thermal stabilities
of 1–4 were studied by TGA on crystalline samples under
an N2 atmosphere with a heating rate of 108CminÀ1 between
room temperature and 5008C. All TG plots of these inclu-
sion compounds exhibited an abrupt weight loss from about
200 to 2158C, that is, the TPTM host is stable up to about
2008C (see Figure S4 in the Supporting Information).
Reversible exchange and separation of guests on single crys-
tals: Compounds 4 have about 24% solvent-accessible
volume per unit cell,[22] which is occupied by diverse guest
molecules. Additionally, the networks of compounds 4 are
expected to have flexibility to some extent because of the
large open channels assembled from purely organic mole-
cules only by interdigitated packing. On the basis of these
considerations, we tested whether the guests can be ex-
changed or selectively adsorbed within the channels in the
vapor phase under mild conditions.
For compound 1, a gradual weight loss of approximately
5.74% from 50 to 1208C corresponds to the loss of the
MeCN molecules (calcd 5.60%), which suggests that the
packing is not close and guest molecules tend to escape
from the voids of the crystal lattice. The TG analysis of 2 in-
dicated three sequential steps of weight loss before collapse
of the host: a gradual weight loss of approximately 2.56%
initially occurs from 86 to 1708C, and then weight losses of
1.36 and 2.25% in the ranges of 171–178 and 182–1908C
correspond to evacuation of the other two kinds of CH2Cl2
molecules (calcd 2.32, 1.16, 2.32%). These stepwise weight
losses of diverse thermal stabilization may correspond to the
three categories of crystallographic positions of dimers in 2.
For compounds 3 with form III, the weight loss up to about
1908C can be assigned to the release of the corresponding
encapsulated guest molecules (calcd for 3a: 6.24%, found:
6.02%; calcd for 3b: 7.12%, found: 7.07%; calcd for 3d:
4.95, found: 4.91%; loss of guest and collapse of the TPTM
host overlap for 3e). For these guest molecules packed in di-
meric capsules of 2 and 3, the escape processes all require
relatively high temperatures and the obvious evacuation
usually occurs after about 1508C. Particularly for 2, the en-
capsulated CH2Cl2 has a low boiling point of 408C but ex-
ceedingly high escape temperatures of about 170 and 1808C.
These results are in good agreement with the structures of
compounds 2 and 3 and demonstrate the outstanding inclu-
sion capability of the TPTM host molecule.
When single crystals of 4a containing benzene molecules
were exposed to toluene vapor at 308C for about 20 d, they
retained single crystallinity, and single-crystal X-ray analysis
gave crystal cell parameters similar to those of 4a. However,
1
the H NMR spectrum indicates that the benzene has been
completely replaced by toluene in a molar host/guest ratio
of approximately 2:1 to generate TPTM·0.5C7H8 (4j; Fig-
ure S6 of the Supporting Information). It is reasonable that
toluene cannot afford a compound with 1:1 host/guest ratio
as observed in compounds 3c–3h (Figure 6b) due to the re-
pelling effect between methyl groups of toluene. Interesting-
ly, the crystal transformation between 4a and 4j is reversi-
ble. Exposing the same batch of crystals 4j to benzene
vapor for about 20 d led to re-adsorption of benzene to
afford 4a’ (Figure S6 of the Supporting Information).
Because the channels in 4 can accommodate substituted
benzenes in an upright fashion along the channels, separa-
tion of linear and branched hydrocarbons, such as xylene
isomers, can be envisioned. To explore the separation of
xylene isomers in the vapor phase, crystals 4a were exposed
to an equimolar mixed vapor of xylene isomers for 20 d at
408C. The 1H NMR spectrum indicated that only the p-
xylene is adsorbed into the channels, displacing the benzene
to generate TPTM·0.25PX (4k) with an approximately 4:1
molar ratio of host/guest (Figure S6 of the Supporting Infor-
mation). Also, the X-ray structural analysis confirms guest
exchange in the channels and the single-crystallinity of 4k.
The crystal transformation between 4a and 4k is reversible,
and compound 4a’’ re-obtained in benzene vapor was char-
acterized by X-ray structural analysis, which indicated that
the guest exchange process could take place in a reversible
single-crystal to single-crystal manner. Apparently, this se-
lective adsorption is due to the diameter of the hexagonal
channel, which can accommodate linear benzene derivatives
and exclude nonlinear ones (Figure 7). This property is rem-
iniscent of the inclusion behavior of urea and thiourea clath-
For compounds 4 with open channels, all guest molecules
are completely removed before collapse of the host (calcd
for 4a: 5.07 and 5.07%, found: 5.17 and 5.01%; calcd for
4e: 18.51, found: 19.10%; calcd for 4g: 17.44, found:
18.21%). As shown for 4a in Figure S4 of the Supporting
Information, TGA indicates that there are two separate
steps of weight loss before collapse of the host at about
2008C, corresponding to loss of two kinds of benzene mole-
cules at 100–123 and 175–1958C. When as-prepared 4a is
treated under vacuum for 24 h, the sample undergoes the
first loss of benzene molecules at 908C, but retains the origi-
nal structure and the second type of benzene molecules. In
contrast, the structure of 4a obviously changes after only 4 h
above 1058C, affording a new unknown phase 4x character-
1
ized by XRPD patterns, although the H NMR spectrum re-
vealed that the second type of benzene molecules still re-
Chem. Eur. J. 2011, 17, 2189 – 2198
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