(3) Formation of Blsol from (P1 + P2) or from Blneat amounts to
a randomization giving a copolymeric material containing all four
monomeric components Am1, Am2, Ald1 and Ald2.
(4) Formation of Blneat from the Blsol random copolymer in the
neat state upon solvent removal amounts to a derandomization
giving a mixture of only the polymers P3d and P4d. This implies a
process of self-selection under the pressure of the formation of an
organized phase, the crystalline copolymer P4.
(5) The system described here represents a constitutional
dynamic material displaying adaptive behavior by constitutional
dynamic interconversion between two constitutional states in
response to a change in physical stimuli (‘‘solution’’ or ‘‘neat’’
conditions).
The present results demonstrate the generation of dynamic
imine polymers displaying constitutional dynamics by reorganiza-
tion and exchange of the monomers in the polymer chains through
bond recombination between their dialdehyde and diamine
components. More importantly, these dynamers can adapt to
different environmental conditions that stabilize/destabilize the
mesoscopic states of the CDL members. Last but not least, the
dynamic selection processes can be reversibly switched over several
interconversion cycles without significant fatigue. In more general
terms, dynamers belong to a class of materials that may respond to
chemical effectors or physical stimuli by constitutional variation,
i.e. adaptive materials.
Scheme 1 Schematic representation of adaptive behavior of the dynamic
polymer system in response to a change in physical state: solution and neat
acting as stimuli.
Notes and references
1 (a) J.-M. Lehn, Chem.–Eur. J., 1999, 5, 2455–2463; (b) J.-M. Lehn and
A. V. Eliseev, Science, 2001, 291, 2331–2332.
2 (a) S. J. Rowan, S. J. Cantrill, G. R. L. Cousins, J. K. M. Sanders and
J. F. Stoddart, Angew. Chem., Int. Ed., 2002, 41, 898–952; (b)
P. T. Corbett, J. Leclaire, L. Vial, K. R. West, J.-L. Wietor, J. K. M.
Sanders and S. Otto, Chem. Rev., 2006, 106, 3652–3711.
3 (a) J.-M. Lehn, Polym. Int., 2002, 51, 825–839J; (b) J.-M. Lehn, Science,
2002, 295, 2400–2403; (c) J.-M. Lehn, Chem. Soc. Rev., 2007, 36,
151–160.
Fig. 4 Photographs taken with
a polarized light microscope in
transmission mode (640) at 80 uC: (a) isotropic phase of homopolymer
P1 at 80 uC, (b) isotropic phase of homopolymer P2 at 80 uC and (c)
anisotropic phase of polymer blend Blneat (P3 + P4) at 80 uC.
4 J.-M. Lehn, Prog. Polym. Sci., 2005, 30, 814–831.
5 (a) T. Ono, S. Fujii, T. Nobori and J.-M. Lehn, Chem. Commun., 2007,
46–48; (b) N. Sreenivasachary, D. T. Hickman, D. Sarazin and
J.-M. Lehn, Chem.–Eur. J., 2006, 8581–8588; (c) N. Giuseppone,
G. Fuks and J.-M. Lehn, Chem.–Eur. J., 2006, 1723–1735; (d) T. Ono,
T. Nobori and J.-M. Lehn, Chem. Commun., 2005, 1522–1524; (e)
W. G. Skene and J.-M. Lehn, Proc. Natl. Acad. Sci. U. S. A., 2004, 101,
8270–8275; (f) N. Giuseppone and J.-M. Lehn, J. Am. Chem. Soc., 2004,
126, 11448–11449.
6 (a) H. Otsuka, K. Aotani, Y. Higaki and A. Takahara, J. Am. Chem.
Soc., 2003, 125, 4064–4065; (b) X. Chen, M. A. Dam, K. Ono, A. Mal,
H. Shen, S. R. Nutt, K. Sheran and F. Wudl, Science, 2002, 295,
1698–1702; (c) K. Oh, K.-S. Jeong and J. S. Moore, Nature, 2001, 414,
889–893.
7 J.-M. Lehn, in Supramolecular science: where it is and where it is going,
ed. R. Ungaro and E. Dalcanale, Kluwer, Dordrecht, 1999, pp. 287–
304.
8 (a) L. Brunsweld, B. J. B. Folder, E. W. Meijer and R. P. Sisjbesma,
Chem. Rev., 2001, 101, 4071–4197; (b) J.-M. Lehn, Polym. Int., 2002, 51,
825–839; (c) Supramolecular Polymers, ed. A. Ciferri, Taylor &
Francis, Boca Raton, 2nd edn, 2005; (d) J.-M. Lehn in ref. 3a ch. 1,
p. 3.
P2, P3 and the mixed polymers existed as isotropic liquids, while
P4 was the only crystalline member. This strong driving force
shifted the equilibria of the CDL towards P4 and, as consequence,
generated also agonistically11 the copolymer P3. As shown in
Fig. 4, both neat parent dynamers, P1 and P2, existed as isotropic
liquids at 80 uC, while an anisotropic phase grew up after stacking
them together in the same conditions. On the other hand, when the
polymer blend Blneat was dissolved in an organic solvent, the
dissolution of the crystalline phase allowed the dynamic system to
re-adapt, reshuffle and re-exchange the monomers so as to
generate the four imine domains of P1, P2, P3 and P4.
The processes described here present several aspects of adaptive
behavior in a system of covalent dynamic polymers in response to
a change in physical state (Scheme 1).
(1) The parent dynamers P1 and P2 generated two offspring
dynamer blends, a random copolymer Blsol when mixed in
solution, and a mixture Blneat of the two polymers P3 and P4 in
neat conditions.
9 (a) J. R. Nitschke and J.-M. Lehn, Proc. Natl. Acad. Sci. U. S. A., 2003,
100, 11970–11974; (b) N. Screenivasachary and J.-M. Lehn, Proc. Natl.
Acad. Sci. U. S. A., 2005, 102, 5938–5943.
10 Synthetic procedures and compounds will be described in detail in a full
paper. All new compounds have been characterized by the usual
spectroscopic and analytical techniques.
(2) This adaptive behavior is retained in the generation of the
offspring systems B1sol and Blneat, which can be reversibly switched
over several dissolution–evaporation cycles.
11 N. Giuseppone and J.-M. Lehn, Chem.–Eur. J., 2006, 12, 1715–1722.
This journal is ß The Royal Society of Chemistry 2007
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