isolated yields in all cases. Surprisingly, in the case of the
reaction employing 1 equivalent each of 3,5-di-tert-butyl
phenylazide and 3,5-di-tert-butyl phenylacetylene (the most
sterically demanding of these substrates) a quantitative yield
1
of [2]rotaxane 6 was observed by H NMR spectroscopy and
an excellent isolated yield (99%) obtained.
Slow evaporation of a saturated solution of [2]rotaxane 6
in Et2O/hexane yielded crystals suitable for single-crystal X-
ray analysis (Figure 3).[14] In addition to the anticipated
CH···N hydrogen bonding interaction between the bipyridine
nitrogens and Hd a number of weak CH···p interactions are
observed between HD and HH and the triazole unit. The
crystal structure clearly shows the extremely sterically con-
gested environment around the triazole unit. Indeed, given
the lack of space within the macrocyclic cavity it seems
surprising that the CuAAC reaction occurs at all, let alone in
the excellent yields obtained.
Figure 4. 1H NMR spectra (400 MHz, CDCl3, 300 K) of rotaxanes a) 5,
b) 6, c) 10, and d) and e) expansions (600 MHz, CDCl3) of the
indicated regions of spectrum (c) demonstrating the rotational dis-
symmetry of the macrocycle. Labeling as shown in Figure 2.
resonances observed which can be assigned to the macrocyclic
component compared with 13 in macrocycle 3b.
The “small” rotaxanes synthesized (Figure 2) demon-
strate a number of important advantages of the CuAAC-AT
approach using smaller macrocycles: 1) operationally trivial
and general access to functionalized rotaxanes with half-
threads derived from commercially available materials such
as simple dialkylbenzene units (5 and 6), benzene rings
bearing single-atom-reactive functionalities (7), trialkyl silyl
units (8), simple flurophores (9), and chiral pool materials
(10) without the need to modify them to include bulky
substituted trityl groups with the concomitant increase in
molecular weight and limitations with respect to solubility
that entails; 2) the ability to use simple aryl azides and
alkynes to generate [2]rotaxanes in which the thread is fully
conjugated (6, 7, and 9) with the potential to extend this
methodology to the synthesis of oligomeric insulated molec-
ular wires;[9] 3) 1H NMR and X-ray crystallographic analysis
of the rotaxane products indicate significantly increased
interaction between macrocycle and thread. In the case of
rotaxane 10 this results in efficient transfer of chiral informa-
tion from the thread to the macrocycle, raising the possibility
of using a chiral-pool-derived, enantiopure thread as a
mechanical chiral auxiliary for achiral macrocyclic ligands in
asymmetric catalysis.[12]
In conclusion, we have demonstrated that it is possible to
vary the size of the macrocycle in the CuAAC-AT reaction
and, by reducing the size of the macrocycle, gain access to
functionalized products in excellent yield. Further, employing
the smallest macrocycle investigated, perhaps surprisingly,
leads to the most efficient active template reaction reported
to date in which an equimolar mixture of macrocycle and half-
thread components leads to a quantitative yield of [2]rotax-
ane product. Work is currently underway to apply these
findings to the synthesis of functional materials and devices.
We are also investigating the effect of macrocycle size on
other AT reactions not only in order to increase their
synthetic utility, but also to determine if the size dependency
of the reaction yield can shed any light on the underlying
mechanism of the process.
Figure 3. Single-crystal X-ray structure[14] of [2]rotaxane 6 viewed along
the thread axis a) in capped sticks representation with selected close
contacts indicated (majority of H atoms omitted for clarity) and b) in
partial space-fill representation. Selected bond lengths (in ꢀ): N1–H31
2.57, N2–H31 2.49, C31–H23 2.99, C31–H12 2.80, N4–H1 2.65,
N4–H4 2.48, N5–H1 2.84, N5–H4 2.65.
1
The H NMR spectra of rotaxanes 5–10 reveal a number
of interesting features (partial 1H NMR spectra for rotaxanes
ꢀ
5, 6, and 10 are shown in Figure 4). Firstly, the triazole C H,
which is already significantly shifted downfield relative to the
free thread in rotaxane 5 (Dd = 0.8 ppm), resonates even
further downfield in rotaxanes 6–10. In the case of rotaxane 6,
Hd appears at 10.5 ppm—a Dd on interlocking of 2.5 ppm
(Figure 2b). Secondly, the desymmetrization of the two faces
of the macrocycle due to the mechanical bond is clearly
visible in the 1H NMR spectra of rotaxanes 5–10, as had
previously been observed for rotaxane 4d. The chiral glucose-
based stopper in rotaxane 10 leads to an even more
complicated 1H NMR spectrum as the macrocycle is now
completely desymmetrized by the mechanical bond: while
macrocycle 3d displays 8 separate 1H resonances, rotaxane 10
exhibits 23 which can be assigned to the macrocyclic
component, indicating a high degree of chiral information
transfer between thread and macrocycle. The same effect is
evident in the 13C NMR spectrum of rotaxane 10 with 25
Angew. Chem. Int. Ed. 2011, 50, 4151 –4155
ꢀ 2011 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
4153