ring with two recognition sites grafted into the other
(nondegenerate) ring can be employed to stimulate the
circumrotation of the first ring around the second one.
Thus, a large-amplitude molecular mechanical motion can
be realized within a mechanically interlocked molecules
be it a [2]catenane or a [2]rotaxanesprovided it exhibits
bistability within the time frame of the experiment in
progress. Further necessary conditions for generating highly
controllable molecular actuations in a bistable [2]rotaxane,
for example, are (i) an appreciable difference in the binding
affinities of the ring component for the two different
recognition sites on the dumbbell component and (ii) a means
of altering completely the binding affinities in a wholly
reversible manner. A free energy difference of greater than
1.2 kcal mol-1 between the two translational isomers of a
bistable rotaxane ensures that, at room temperature, at least
90% of the molecules have the ring residing around one site
in preference to the other one. In order to induce motion of
the ring along the dumbbell component within such bistable
rotaxanes, a variety of stimulise.g., chemical, electrochemi-
cal, and photochemicalshave been employed3,4 with con-
siderable success. In the case of MEDs,3 successful device
performance has also been asscociated with a free energy
barrier in excess of 21 kcal mol-1 between the translational
isomers where the so-called metastable state co-conformation
(MSCC) and the ground-state co-conformation (GSCC)
corresponding to the ON and OFF states, respectively of the
switch.
advent more recently6 of the copper(I)-catalyzed azide-alkyne
cycloaddition7 (CuAAC) has made it possible to synthesize
(Scheme 1) a bistable [2]catenane 1·2PF6 with a much larger
Scheme 1. Synthesis of the [2]Catenane 1·2PF6
In the past, bistable donor-acceptor [2]catenanes have been
sythesized by a template-directed protocol5 in which the
recognition sites in one ring act as a template for the
formation of the mechanically interlocked second ring. The
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M. C.; Sauvage, J.-P. Acc. Chem. Res. 2001, 34, 477–487. (b) Kim, K.;
Jeon, W. S.; Kang, J.-K.; Lee, J. W.; Jon, S. Y.; Kim, T.; Kim, K. Angew.
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free energy barrier between its MSCC and GSCC, while
hopefully retaining the free energy difference between the
two translational isomers. This communication describes the
synthesis, employing CuAAC, of 1·2PF6 and the character-
ization of the bistable [2]catenane using 1H NMR spectros-
copy and cyclic voltammetry in (CD3CN/MeCN) solution.
The synthesis of 1·2PF6, which is composed of a π-electron
rich bis-1,5-dioxynaphthalene[38]crown-10 (BDNP38C10)
ring mechanically interlocked with a second macrocycle
containing two π-electron-deficient recognition sitessnamely,
a naphthalene diimide (NpI) unit and a 4,4′-bipyridinium
(BIPY2+) oneswhich are separated by two bulky tetraaryl-
methane residues, designed to act as “speed bumps”, is
outlined in Scheme 1. The tetraarylmethane derivative 2,
carrying a tosyl group at one end and a hydroxyl group at
the other, was prepared according to the literature.8 The NpI
derivative 3 was isolated in 82% yield, after carrying out a
Mitsunobu reaction between NpI and 2 in the presence of
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ˇ
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