893
through a simple enlargement of the ends (Table 1, Entry 5). Also, an
expanding reaction at room temperature failed to hold a ring even
after maintaining the system at 60 °C for 7 days (Table 1, Entry 6).
These results are interesting in terms of controlling the content of
cyclic molecules in a CD-based polyrotaxane. In some cases, especially
for polymeric chains with large molecular weights, self-assembly of
cyclic molecules onto a long polymeric chain can lay down in the
course of threading to give a partially covered pseudopolyrotaxane as a
solid, which is not always arbitrarily controlled by mixing conditions
such as ratios, concentrations, temperatures, and others.
In conclusion, we demonstrated a synthetic approach, the
slipping-expanding protocol, for the construction of a loose-fit
polyrotaxane, based on the complexation between mismatched
components of ¢-CD and PEG derivatives, followed by enlargement
of the ends of PEG through a chemical modification. The protocol, in
principle, would be applied to a wide variety of polyrotaxane
preparations. When the ¢-CD derivative is linked by a spacer, self-
assembly of the linked derivative onto the dumbbell-shaped PEG at
an elevated temperature would be also interesting in terms of
designing a novel class of thermoresponsive materials, which is in
progress and will be reported soon.
The authors thank Associate Prof. Akio Ohta (Kanazawa
University) and Dr. Issey Osaka (JAIST) for their help in character-
ization (elemental analysis and mass spectroscopy) of the new
componds.12
Figure 1. 1H NMR spectra (400 MHz) of (a) dumbbell 4, (b) ring 2, and
(c) polyrotaxane 3 (Entry 3), measured in CDCl3 at room temperatrue.
References and Note
1
2
3
4
a) M. Asakawa, P. R. Ashton, R. Ballardini, V. Balzani, M. Bĕlohradský,
M. T. Gandolfi, O. Kocian, L. Prodi, F. M. Raymo, J. F. Stoddart, M.
M. C. T. Fyfe, F. M. Raymo, N. Spencer, J. F. Stoddart, A. J. P. White, D. J.
J. S. Hannam, S. M. Lacy, D. A. Leigh, C. G. Saiz, A. M. Z. Slawin, S. G.
Table 1. Conditions for slipping, the number (m) of 2 in 3, determined by
1H NMR, and yields of 3a
Entry
Temp/°C
Time/day
m
Yield of 3/%
1
2
3
4
5
6
60
60
60
60
rt
3
7
14
21
14
7
1.0
2.5
3.4
3.6
®
17
14
14
14
<1
<1
60
®
aConcentrations of 1 and 2 were constant ([1] = 6 © 10¹2 M and
[2] = 7 © 10¹1 M). Mixing at lower concentrations ([1] < 3 ©10¹2 M
and [2] < 4 © 10¹1 M) failed to give 3. The yields of 3 were calculated
based on 1 with an assumption that the repeating distribution of an
ethylene glycol unit in 1 (averaged n = 24) was invariable. Conditions
for the expanding reaction are as follows: BnN3 (10 equiv), CuSO4
(0.8 equiv), and (+)-ascorbic acid (2 equiv), for 3 h at the same
temperature as in the slipping process (Entries 1-5) and rt (Entry 6).
5
6
7
8
Mixing of 1 and 2 in water at 25/60 °C led to no change in
appearance due to high water-solubility of 2,11 thus the transparent
solution was subjected to the expanding reaction in one pot after a
period of slipping to give loose-fit polyrotaxanes 3 in 14-17% yield,
which was successfully isolated in pure form by silica gel column
chromatography and gel permeation chromatography due to the
differences in Rf value (0.44 for 3, 0.36 for 4, and 0.09 for 2, eluted
with 10% MeOH/CH2Cl2 on SiO2) and retention time (see
experimental section and Figure S1).12 The ¢-CD derivative 2 was
found in association with a PEG component in the 1H NMR spectrum
of 3 exhibiting a simple integration of each component (Figure 1).
The content of 2 in a series of 3 was increased with time for slipping
(Table 1, Entries 1-4). Isolation of polyrotaxanes 3 can support the
slipping and entrapping of 2 onto 1 in water at 60 °C. It is noted that
the slipping and expanding reaction at room temperature did not lead
to a sufficient amount of rotaxane, but gave a dumbbell 4 in 88% yield
9
I. W. Muderawan, T. T. Ong, T. C. Lee, D. J. Young, C. B. Ching, S. C. Ng,
11 The 1H NMR spectrum of 1 itself ([1] = 3.2 © 10¹2 M) measured in D2O at
room temperature showed broadened resonances, whose intensity was
remarkably increased at 60 °C, although the solution remained turbid in
appearance at both temperatures due to the hydrophobic inherence in 1. No
difference was found in the spectra of 2 itself ([2] = 3.5 © 10¹1 M)
measured in D2O at both temperatures, exhibiting sharpened resonances.
Upon mixing of them in D2O, significant downfield shifts were induced for
the protons of terminal group in 1, which were observed at both
temperatures. The intensity of the resonances was unchanged in the two
spectra measured at room temperature and 60 °C, unlike in the case of 1
itself.
12 Supporting Information is available electronically on the CSJ-Journal Web
Chem. Lett. 2010, 39, 892-893
© 2010 The Chemical Society of Japan