0.1305 (all data). Carbonyl groups assigned by C–O bond lengths. CCDC
graphic files in .cif or other format.
‡ Crystal data for 2: C14H10NO5, M = 258.23, monoclinic, space group C2/
c (no. 15), a = 13.5889 (5), b = 6.6994 (3), c = 13.5648 (6) Å, V =
1217.39 (9) Å3, T = 298 K, Z = 4, m = 0.11 mm21, 1972 reflections
To test our ability to control the carboxylic acid conforma-
tion, we synthesized 2 using a copper-catalyzed ether coupling
of o-methylphenol and o-iodotoluene, previously reported by
our group,9 followed by oxidation with KMnO4.10 We
hypothesized that the ether linkage would hydrogen-bond with
one of the acidic hydrogens, resulting in the asymmetric
conformation. Unfortunately, single crystal X-ray diffraction of
2‡ (Fig. 3b) reveals that both carbonyls are facing in the same
direction, resulting in a similar zig-zag structure as seen in 1,
except the conformation of the carboxylic acids are completely
reversed. We hypothesize that the carboxyl hydrogens are
slightly disordered such that one occupies the three-oxygen
cavity for some percentage of time in the solid-state (Fig. 2),11
thus providing stabilization for this conformation.
In order to achieve the desired assymmetric conformation, we
synthesized 3 through an Ullmann coupling,§ followed by
simple base hydrolysis and recrystallization from a water–
acetone mixture. Single crystal X-ray diffraction shows that 3¶
obtains an asymmetric conformation except the intermolecular
hydrogen bonds are not dimeric. This is due to the internal
hydrogen-bonds between the two carboxylic acids as well as the
tertiary amine (Fig. 2). Moreover, 3 is observed to self-assemble
into a supramolecular helix (Fig. 3c) as predicted by packing
motif III. It should be noted that both the right-handed and left-
handed helices are present in the unit cell. It is also important to
note that solvent water does not interfere in the assembly of this
helical structure, a common problem in supramolecular chem-
istry due to competition by the protic solvent for hydrogen
bonds.12
As discussed previously, motif II is less favoured due to
inefficient inter-stack packing, but it also forms a more rigid and
a less efficient coil (more residues per length) than motif III.
More difficult to explain is the absence of the zig-zag motif (I),
which facilitates packing between stacks. The angle between
the planes of the two benzoic acid rings are approximately 44°,
66°, and 81° corresponding to compounds 1, 2, and 3,
respectively. The more open angle of 3, combined with its
bonding conformation, may give rise to the helical assembly
over the zig-zag structure. It is also possible that the bulk of the
additional phenyl group in 3 is better accommodated by the
helical motif in this case.
measured, 1057 unique (Rint = 0.031), R1 = 0.0632 (all data)], wR2
=
0.1455 (all data). Carbonyl groups assigned by C–O bond lengths. CCDC
173737.
§ Aniline (2.28 mL, 25 mmol), methyl-2-iodobenzoate (11.18 mL, 52.5
mmol), K2CO3 (7.26 g, 52.5 mmol), Cu (0.33 g, 5.2 mmol), and CuI (0.22,
1.2 mmol) combined in 20 mL di-n-butyl ether and refluxed under argon for
48 h. Column chromatography (4+1, hexane–ethyl acetate) followed by
recrystallization from ethanol gave the coupled product in 81% yield. Base
hydrolysis with NaOH in EtOH–H2O (1+1) gave 3 in 99% conversion.
Crystals were obtained from slow evaporation of an acetone–water solution
of 3.
¶ Crystal data for 3: C20H15NO4, M = 333.34, monoclinic, space group
P21/c (no. 14), a = 9.2755 (2), b = 10.7912 (4), c = 16.7186 (4) Å, V =
1658.61 (8) Å3, T = 298 K, Z = 4, m = 0.09 mm21, 5471 reflections
measured, 2901 unique (Rint = 0.034), R1 = 0.0539 (all data), wR2
=
0.1138 (all data). Carbonyl groups assigned by C–O bond lengths. CCDC
173738.
1 For general reviews see: (a) A. E. Rowan and R. J. M. Nolte, Angew.
Chem., Int. Ed., 1998, 37, 63; (b) D. S. Lawrence, T. Jiang and M.
Levett, Chem. Rev., 1995, 95, 2229; (c) A. P. Alivisatos, P. F. Barbara,
A. W. Castleman, J. Chang, D. A. Dixon, M. L. Klein, G. L. McLendon,
J. S. Miller, M. A. Ratner, P. J. Rossky, S. I. Stupp and M. E. Thompson,
Adv. Mater., 1998, 10, 1297.
2 For specific examples of helical architectures see: (a) C. Nuckolls, T. J.
Katz, G. Katz, P. J. Collings and L. Castellanos, J. Am. Chem. Soc.,
1999, 121, 79; (b) T. B. Norsten, R. McDonald and N. R. Branda, Chem.
Commun., 1999, 8, 719; (c) P. Gangopadhyay and T. P. Radhakrishnan,
Angew. Chem., Int. Ed., 2001, 40, 2451; (d) S. J. Geib, G. Vicent, E. Fan
and A. D. Hamilton, Angew. Chem., Int. Ed., 1993, 32, 119; (e) M. J.
Marsella, I. T. Kim and F. Tham, J. Am. Chem. Soc., 2000, 122, 974; (f)
K. Hanabusa, M. Yamada, M. Kimura and H. Shirai, Angew. Chem., Int.
Ed., 1996, 35, 1949; (g) S. Hanessian, M. Simard and S. Roelens, J. Am.
Chem. Soc., 1995, 117, 7630; (h) O.-S. Jung, Y. J. Kim, Y.-A. Lee, J. K.
Park and H. K. Chae, J. Am. Chem. Soc., 2000, 122, 9921.
3 G. R. Desiraju, Angew. Chem., Int. Ed., 1995, 34, 2311.
4 L. Leiserowitz, Acta Cryst. Sec. B, 1976, 32, 775.
5 C. Bilton, F. H. Allen, G. P. Shields and J. A. K. Howard, Acta Cryst.
Sec. B, 2000, 56, 849.
In summary, we have reported a novel molecular system in
which the conformation of the intermolecular hydrogen-
bonding, and thus the supramolecular structure, can be
controlled through an internal hydrogen-bond. This work is an
example of a rational design approach for assembling predict-
able molecular architectures that may potentially lead to
functional materials with interesting solid-state properties.13
The triphenylamine moiety may also assist in the development
of such materials.14 Studies are under way to determine if these
molecules aggregate in the solution phase.
6 (a) Y. Ducharme and J. D. Wuest, J. Org. Chem., 1988, 53, 5789; (b) E.
Boucher, M. Simard and J. D. Wuest, J. Org. Chem., 1995, 60, 1408; (c)
L. Vaillancourt, M. Simard and J. D. Wuest, J. Org. Chem., 1998, 63,
9746.
7 Intramolecular hydrogen bonds have been used to control helical
conformations in oligomers. See (a) J. Zhu, R. D. Parra, H. Zeng, E.
Skrzypczak-Jankun, X. C. Zeng and B. Gong, J. Am. Chem. Soc., 2000,
122, 4219; (b) Y. Hamuro, S. J. Geib and A. D. Hamilton, J. Am. Chem.
Soc., 1997, 119, 10587.
8 R. Gujadhur, D. Venkataraman and J. T. Kintigh, Tetrahedron Lett.,
2001, 42, 4791.
Financial support for this research was provided by the
University of Massachusetts, Amherst start-up funds. We thank
the X-ray Structural Characterization Laboratory supported by
National Science Foundation grant CHE-9974648 for collecting
single crystal data for 1, 2 and 3. DV gratefully acknowledges
the Camille and Henry Dreyfus New Faculty Award.
9 R. Gujadhur and D. Venkataraman, Synth. Commun., 2001, 31, 2865.
10 R. Shapiro and D. Slobodin, J. Org. Chem., 1969, 34, 1165.
11 Although not conclusive, X-ray diffraction shows some residual
electron density where the disordered proton is expected.
12 (a) G. M. Whitesides, J. P. Mathias and C. T. Seto, Science, 1991, 254,
1312; (b) G. R. Desiraju, J. Chem. Soc., Chem. Commun., 1991, 426; (c)
J. H. K. Ky Hirschberg, L. Brunsveld, A. Ramzi, J. A. J. M. Vekemans,
R. P. Sejbesma and E. W. Meijer, Nature, 2000, 407, 167.
13 Helical systems are candidates for circularly polarized light emitters.
See M. Grell and D. C. D. Bradley, Adv. Mater., 1999, 11, 895.
14 Triphenylamines are widely exploited as materials for display applica-
tions. See E. Bellmann, S. E. Shaheen, S. Thayumanavan, S. Barlow, R.
H. Grubbs, S. R. Marder, B. Kippelen and N. Peyghambarian, Chem.
Mater., 1998, 10, 1668 and references contained therein.
Notes and references
† Crystal data for 1: C14H11NO4, M = 251.27, monoclinic, space group C2/
c (No. 15), a = 13.1691 (7), b = 8.3651 (5), c = 11.7215 (5) Å, V =
1208.38 (11) Å3, T = 298 K, Z = 4, m = 0.11 mm21, 2456 reflections
measured, 1387 unique (Rint = 0.027), R1 = 0.0582 (all data), wR2
=
CHEM. COMMUN., 2002, 306–307
307