C O M M U N I C A T I O N S
Table 1. Kinetic and Thermodynamic Parameters for the
Conversion of 2in- [1⊃2][PF6]6 to 3in-[1⊃2][PF6]6
References
k1a
k2a
K
∆G qThinSpaceb
∆G q b
∆G
b
1
2
(1) (a) Balzani, V.; Credi, A.; Raymo, F. M.; Stoddart, J. F. Angew. Chem.,
Int. Ed. 2000, 39, 3343-3391. (b) Leigh, D. A.; Wong, J. K. Y.; Dehez,
F.; Zerbetto, F. Nature 2003, 424, 174-179. (c) Balzani, V.; Credi, A.;
Venturi, M. Molecular DeVices and Machines: A Journey into the Nano
World; Wiley-VCH: Weinheim, Germany, 2003.
4.7 ( 0.1 1.4 ( 0.1 3.4 ( 0.1 20.9 ( 0.3 21.5 ( 0.3 -0.60 ( 0.01
a
b
In s-1 × 106. In kcal mol-1
.
(2) (a) Wisner, J. A.; Loeb, S. J. Angew. Chem., Int. Ed. 1998, 37, 2838-
2840. (b) Huang, F.; Gibson, H. W.; Bryant, W. S.; Negvekar, D. S.;
Fronczek, F. R. J. Am. Chem. Soc. 2003, 125, 9367-9371. (c) Davidson,
G. J. E.; Loeb, S. J. Angew. Chem., Int. Ed. 2003, 42, 74-77.
(3) (a) Mammen, M.; Choi, S.-K.; Whitesides, G. M. Angew. Chem., Int. Ed.
1998, 37, 2754-2794. (b) Gestwicki, J. E.; Cairo, C. W.; Strong, L. E.;
Oetjen, K. A.; Kiessling, L. L. J. Am. Chem. Soc. 2002, 124, 14922-
14933. (c) Kitov, P. I.; Bundle, D. R. J. Am. Chem. Soc. 2003, 125,
16271-16284. (d) Ercolani, G. J. Am. Chem. Soc. 2003, 125, 16097-
16103.
of resonances to a single 1:1 complex with averaged C3V symmetry,
i.e., 3in-[1⊃2][PF6]6. The resonances of the central aromatic core
protons, namely Ha in [1][PF6]6 and Hm in 2, showed significant
upfield shifts, compared to the corresponding resonances of the
free components (Figure 2a,d), indicating intimate π-π stacking9,11
of the central aromatic cores. The previously enantiotopic OCH2
protons in 2 (Figure 2a) become diastereotopic in 3in-[1⊃2][PF6]6
(Figure 2c) when all three bipyridinium units became threaded
through the crown ether moieties. Furthermore, the resonances for
the six equiValent R-bipyridinium He protons in 3in-[1⊃2][PF6]6
(Figure 2c) are dramatically shifted, as compared to the signals
for these same protons in [1][PF6]6 (Figure 2a) as a result of
[CR-H‚‚‚O] interactions.12 The single resonance for the Me protons
in 3in-[1⊃2][PF6]6 (Figure 2c) also confirms the binding of all three
bipyridinium units.
(4) (a) Whitesides, G. M.; Mathias, J. P.; Seto, C. T. Science 1991, 254, 1312-
1319. (b) Wintner, E. A.; Conn, M. M.; Rebek, J., Jr. Acc. Chem. Res.
1994, 27, 198-203. (c) Crego-Calama, M.; Reinhoudt, D. N. Science 2002,
295, 2403-2407.
(5) Fulton, D. A.; Cantrill, S. J.; Stoddart, J. F. J. Org. Chem. 2002, 67, 7968-
7981 and references therein.
(6) (a) Rao, J.; Lahiri, J.; Isaacs, L.; Weis, R. M.; Whitesides, G. M. Science
1998, 280, 708-711. (b) Kitov, P. I.; Sadawska, J. M.; Mulvey, J. P.;
Armstrong, G. D.; Ling, H.; Pannu, N. S.; Read, R. J.; Bundle, D. R.
Nature 2000, 403, 669-672. (c) Gibson, H. W.; Yamaguchi, N.; Hamilton,
L.; Jones, J. W. J. Am. Chem. Soc. 2002, 124, 4653-4665.
(7) Ashton, P. R.; Ballardini, R.; Balzani, V.; Credi, A.; Dress, K. R.; Ishow,
E.; Kleverlaan, C. J.; Kocian, O.; Preece, J. A.; Spencer, N.; Stoddart, J.
F.; Venturi, M.; Wenger, S. Chem. Eur. J. 2000, 6, 3558-3574.
(8) 1,3,5-Tris(p-formylphenyl)benzene was reduced initially with NaBH4 to
1,3,5-tris(p-hydroxybenzyl)benzene, followed by chlorination with N-
chlorosuccinimide to yield 1,3,5-tris(p-chlorobenzyl)benzene. Further
reaction with 4,4′-bipyridine, followed by anion exchange, produced [6]-
[PF6]3, which was then reacted with p-methylbenzyl bromide to yield [1]-
[PF6]6 after anion exchange. For further details, see Supporting Informa-
tion.
(9) (a) Fyfe, M. C. T.; Lowe, J. N.; Stoddart, J. F.; Williams, D. J. Org. Lett.
2000, 9, 1221-1224. (b) Balzani, V.; Clemente-Leon, M.; Credi, A.;
Lowe, J. N.; Badjic´, J. D.; Stoddart, J. F.; Williams, D. J. Chem. Eur. J.
2003, 9, 5348-5360.
(10) (a) Ashton, P. R.; Langford, S. J.; Spencer, N.; Stoddart, J. F.; White, A.
J. P.; Williams, D. J. Chem. Commun. 1996, 1387-1388. (b) Ashton, P.
R.; Glink, P. T.; Mart´ınez-D´ıaz, M. V.; Stoddart, J. F.; White, A. J. P.;
Williams, D. J. Angew. Chem., Int. Ed. Engl. 1996, 35, 1930-1933.
(11) (a) Hunter, C. A.; Sanders, J. K. M. J. Am. Chem. Soc. 1990, 112, 5525-
5534. (b) Adams, H.; Hunter, C. A.; Lawson, K. R.; Perkins, J.; Spey, S.
E.; Urch, C. J.; Sanderson, J. M. Chem. Eur. J. 2001, 7, 4863-4877.
(12) (a) Desiraju, G. R. Acc. Chem. Res. 1991, 24, 290-296. (b) Raymo, F.
M.; Bartberger, M. D.; Houk, K. N.; Stoddart, J. F. J. Am. Chem. Soc.
2001, 123, 9264-9267. (c) Steiner, T. Angew. Chem., Int. Ed. 2002, 41,
48-76.
(13) At temperatures below 253 K, an equimolar mixture (8.5 mM) of 4,4′-
dibenzylbipyridinium bis(hexafluorophosphate) and DB24C8 in CD3-
COCD3 reveals peaks in the 1H NMR spectra for the 1:1 complex as well
as for the free species, i.e., complexation-decomplexation is slow on the
NMR timescale. Thus, it is not surprising that 2in-[1⊃2][PF6]6 is
kinetically stable at 253 K.
(14) The experimental data points were fitted to a model for the reversible
first-order reaction by nonlinear square fitting using SigmaPlot 8.0
software. For further details, see: Espenson, J. H. Chemical Kinetics and
Reaction Mechanisms; McGraw-Hill: New York, 1995; Chapter 3.
(15) For some further examples of strict self-assembly, see: (a) Zimmerman,
S. C. Science 1997, 276, 543-544. (b) Conn, M. M.; Rebek, J., Jr. Chem.
ReV. 1997, 97, 1647-1668. (c) Fujita, M. Acc. Chem. Res. 1999, 32,
53-61. (d) Lehn, J.-M. Proc. Natl. Acad. Sci. U.S.A. 2002, 99, 4763-
4768. (e) Felix, O.; Crego-Calama, M.; Luyten, I.; Timmerman, P.;
Reinhoudt, D. N. Eur. J. Org. Chem. 2003, 8, 1463-1474.
(16) By comparison (ref 9), a trifurcated trisammonium salt, wherein the three
bipyridinium units in [1][PF6]6 are replaced by three CH2NH2+CH2 units,
forms a triply threaded superbundle with 2 instantaneously. No intermedi-
ates are observed on the laboratory timescale. We suspect that the
difference in the rates of formation of the two superbundles can be traced
back to the relative rigidity of [1]6+ compared with its trisammonium-
based analogue.
1
The change in the H NMR spectrum of an equimolar mixture
of [1][PF6]6 and 2, each 5.5 mM, at 253 K with time (235 h) was
monitored (Supporting Information) by 1H NMR spectroscopy. The
concentration of the initially formed 2in-[1⊃2][PF6]6 decreases,
while the concentration of 3in-[1⊃2][PF6]6 increases. When the
concentration of the initially formed 2in-[1⊃2][PF6]6 was plotted
versus time and the data points were fitted (Supporting Information)
to the model for a reversible first-order rate reaction, good
agreement was found.14 This finding supports the evidence for the
presence of two species, i.e., 2in-[1⊃2][PF6]6 and 3in-[1⊃2][PF6]6,
in admixture and slowly equilibrating. The calculated rate constants
for the forward (k1) and backward (k2) reactions and the corre-
q
sponding free energies (∆G1q and ∆G2 ) are presented in Table 1.
The high energy barrier (20.9 kcal mol-1) for the formation of 3in-
[1⊃2][PF6]6 suggests that the initial rapid formation of 2in-[1⊃2]-
[PF6]6 is followed by a much slower binding step, during which
time the third and uncomplexed bipyridinium arm is appropriately
positioned such that the final threading process can take place. The
singly threaded complex 1in-[1⊃2][PF6]6 is most certainly being
formed along the way. Presumably, however, the relatively short
lifetime of this 1:1 complex does not allow us to detect it by
conventional NMR spectroscopy.
In conclusion, we have discovered that the strict self-assembly4,15
of a two-component triply threaded superbundle 3in-[1⊃2][PF6]6
from its components in solution is very much a two-step process,16
with the first one being kinetically and the second one thermo-
dynamically controlled. This observation begs the important ques-
tion: are there instances17 in nature where multivalency is expressed
as a kinetically controlled process, prior to an equilibrium state
being reached and, if so, what are the biological consequences, if
any?
(17) Indeed, there are instances in nature, e.g., a recent study carried out on
the high-avidity, reversible low-affinity multivalent interactions of the
lectin XL35 with the jelly coat proteins surrounding oocytes in Xenopus
laeVis shows that they require a very long time to reach equilibrium, so
long in fact that the partners do not attain true equilibrium on the timescale
of the biological event, namely polyspermy, yet are such that their
metastable mode of interaction is probably more than enough to guarantee
an insurmountable physical block to polyspermy. See: Arranz-Plaza, E.;
Tracy, A. S.; Siriwardena, A.; Pierce, J. M.; Boons, G.-J. J. Am. Chem.
Soc. 2002, 124, 13035-13046.
Acknowledgment. We thank Alshakim Nelson and Scott
Vignon for useful discussions. This research was supported by an
NSF grant (CHE 0317170) and also in part by two equipment grants
(CHE 9974928 and CHE 0092036), also from the NSF.
Supporting Information Available: Experimental details for the
synthesis of [1][PF6]6, 1H-1H COSY, TROESY 2D NMR spectra of
2in-[1⊃2][PF6]6 and 3in-[1⊃2][PF6], and rate constant measurements
(PDF). This material is available free of charge via the Internet at
JA0395285
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