J . Org. Chem. 1999, 64, 4555-4559
4555
Deep er Ca vita n d s
toluene, and the corresponding phenylenediamine units
were condensed with 1,2-diketones. The resulting fused
pyrazines provide the deepened cavities. Diethyl 2,3-
dioxosuccinate and acenaphthenequinone formed cav-
itands 6 and 7, respectively, as yellow solids in 13 and
Fabio C. Tucci, Dmitry M. Rudkevich, and
J ulius Rebek, J r.*
9
The Skaggs Institute for Chemical Biology and Department
of Chemistry, The Scripps Research Institute, 10550 North
Torrey Pines Road, La J olla, California 92037
4
9% (Scheme 1). Lehn and others utilized a similar
heterocyclization strategy to construct helicates and
extended surfaces.10
Received February 3, 1999
The new cavitands 6 and 7 exist in solution as vase-
like C4v structures, as shown by the H NMR spectra in
1
Cavitands are synthetic structures with curved, open-
ended cavities.1 The earliest cavitands were shallow,
bowl-shaped structures 1a ,b prepared from resorcin-
arenes 2 through alkylation or silylation of the phenolic
hydroxyls (Figure 1).2 These cavitands are limited by
their dimensionssca. 9.0 Å wide and 3.0 Å deepsto
various solvents (Figure 2). Only one set of signals was
found for all groups of protons. However, unlike the rigid
cavitand 3, conformational dynamics were observed, in
a process that is intermediate in rate on the NMR time
,3
1
scale (Figure 3). The H NMR spectrum of cavitand 6 in
CDCl
aromatic ring C-H
warmed to 330 K, the H
3
at 295 K displays sharp resonances except for the
(Figure 2). When the sample is
resonance emerges. Similarly,
interact only with small molecules: CH
and CH
2
Cl
CtCH3 are weakly bound by them in solution.
3
2 3 2
, CHCl , CS ,
c
a-d
c
Subsequently, the rims were built up and the cavities
deepened; 3, for example, offers a depth of ∼8.0 Å. Its
binding properties have been examined under a variety
cavitand 7, with its much deeper cavity, displayed broad
resonances at 295 K in a variety of solvents (p-xylene-
d
6 8 3
10, benzene-d , toluene-d , CDCl ). Again, when the
3
-6
of conditions including on solid surfaces.
Cavitand 3a
samples were heated (>330 K), sharp spectra character-
istic of C4v symmetry arose (Figure 2).
complexed simple aromatic molecules.4 We have now
developed access to even deeper cavitands, capable of
housing more sizable guests, and we communicate our
methods here.
Functional group manipulations on the upper rim of 6
were uneventful. The eight ester groups are moderately
activated and underwent conversion to the octacarbox-
amide 8 on treatment with an excess of n-butylamine in
boiling ethanol. The presence of eight hydrogen bond
donor and acceptor sites (the C(O)-NH functions) of 8
imparted a unique, strongly solvent- and temperature-
dependent folding-unfolding behavior that will be de-
scribed elsewhere. Saponification of 6 with aqueous LiOH
resulted in quantitative conversion to the octaacid 9.
The deeper cavitands 3 are usually prepared by bridg-
ing the resorcinarene hydroxyl groups of 2a with a
preformed heterocycle, e.g., condensation with a 6,7-
disubstituted-2,3-dichloroquinoxaline. The alternative
involves the use of a simpler building block in the
bridging reaction and then extension of the rim through
heterocyclic synthesis. Specifically, the octanitro cavitand
7
4
was obtained by reaction of 2a with 1,2-difluoro-4,5-
a
The NMR chemical shifts of the bridging methines (H ,
8
dinitrobenzene in DMF at 70 °C in the presence of Et
3
N.
Figure 2) in cavitands have been used to estimate the
degree of their conformational mobility.3 Methine chemi-
cal shifts above 5.5 ppm indicate a stable “vase” confor-
mation of C4v symmetry, while shifts below 4.0 ppm are
characteristic of the “kite” conformation. The latter has
the four rim aromatics flipped outward and features C2v
symmetry. The conformational preferences are affected
by solvation, dimerization, and complexation and can be
diagnosed by the shift of the CH triplet resonance.
Table 1 records the effect of solvent on this signal for
The NO groups were hydrogenated with Ra/Ni in
2
e
(
1) (a) Cram, D. J . Science 1983, 219, 1177-1183. (b) Cram, D. J .;
Cram, J . M. Container Molecules and their Guests; Royal Society of
Chemistry: Cambridge, 1994; pp 85-130.
(
2) (a) H o¨ gberg, A. G. S. J . Am. Chem. Chem. 1980, 102, 6046-
6
050. (b) H o¨ gberg, A. G. S. J . Org. Chem. 1980, 45, 4498-4500. (c)
Tunstad, L. M.; Tucker, J . A.; Dalcanale, E.; Weiser, J .; Bryant, J . A.;
Sherman, J . C.; Helgeson, R. C.; Knobler, C. B.; Cram, D. J . J . Org.
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(3) (a) Cram, D. J .; Karbach, S.; Kim, H.-E.; Knobler, C. B.;
Maverick, E. F.; Ericson, J . L.; Helgeson, R. C. J . Am. Chem. Soc. 1988,
the new cavitands. In contrast to 3a (R ) C11
molecules 6 and 7 exhibit a very solvent-dependent
methine (H ) chemical shift. The CH triplet of 3a is found
at 5.5 ppm at room temperature in CDCl , while for 6
H23),
1
10, 2229-2237. (b) Cram, D. J .; Stewart, K. D.; Goldberg, I.;
Trueblood, K. N. J . Am. Chem. Soc. 1985, 107, 2574-2575. (c) Tucker,
J . A.; Knobler, C. B.; Trueblood, K. N.; Cram, D. J . J . Am. Chem. Soc.
a
1
989, 111, 3688-3699. (d) Moran, J . R.; Karbach, S.; Cram, D. J . J .
3
Am. Chem. Soc. 1982, 104, 5826-5828. (e) Moran, J . R.; Ericson, J .
L.; Dalcanale, E.; Bryant, J . A.; Knobler, C. B.; Cram, D. J . J . Am.
Chem. Soc. 1991, 113, 5707-5714. (f) Cram, D. J .; Choi, H. J .; Bryant,
J . A.; Knobler, C. B. J . Am. Chem. Soc. 1992, 114, 7748-7765.
and 7 it is located upfield 4.6 ppm. In aromatic solvents,
the methine signal for cavitand 3a is found at ca. 6.0
ppm, while for cavitand 6 the CH triplet is detected at
ca. 4.5 ppm and for 7 it is between 5.4 and 6.0 ppm. The
same trend is observed at higher temperatures (>330 K).
These suggest that the cavities of 6 and 7 are quite
conformationally flexible (Figure 3) and prefer aromatic
solvent molecules.
(4) (a) Dalcanale, E.; Soncini, P.; Bacchilega, G.; Ugozzoli, F. J .
Chem. Soc., Chem. Commun. 1989, 500-502. (b) Soncini, P.; Bonsig-
nore, S.; Dalcanale, E.; Ugozzoli, F. J . Org. Chem. 1992, 57, 4608-
4
612. (c) Dalcanale, E.; Costantini, G.; Soncini, P. J . Inclusion Phenom.
Mol. Recognit. Chem. 1992, 13, 87-92.
5) Gas-phase complexation studies: (a) Vincenti, M.; Dalcanale, E.;
Soncini, P.; Guglielmetti, G. J . Am. Chem. Soc.. 1990, 112, 445-447.
b) Vincenti, M.; Minero, C.; Pelizzetti, E.; Secchi, A.; Dalcanale, E.
(
(
Pure Appl. Chem. 1995, 67, 1075-1084. (b) Dickert, F. L.; Baumler,
U. P. A.; Stathopulos, H. Anal. Chem. 1997, 69, 1000-1005.
(8) Kazimierczuk, Z.; Dudycz, L.; Stolarski, R.; Shugar, D. Nucleo-
sides Nucleotides 1981, 8, 101-117.
(6) Schierbaum, K. D.; Weiss, T.; Thoden van Velzen, E. U.;
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7) (a) Rudkevich, D. M.; Hilmersson, G.; Rebek, J ., J r. J . Am. Chem.
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1
150.
(
(10) (a) W a¨ rnmark, K.; Thomas, J . A.; Heyke, O.; Lehn, J . M. Chem.
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1
0.1021/jo990209z CCC: $18.00 © 1999 American Chemical Society
Published on Web 05/12/1999