.
Angewandte
Communications
we have solved the structure of the
polymer 2 by single-crystal XRD. The
X-ray diffraction pattern of the polymer
2 was very sharp and clear, similar to
that of monomer 1. It is noteworthy that
the crystal structure could be refined to
a very good R-Factor (2.98) suggestive
of the highly homogeneous nature of
the polymer in the crystal. Interestingly,
the space group of the polymer was
same (P212121) as that of the monomer
1. The polymerization resulted in slight
change of unit cell parameters. While
“a” (4.718 ꢀ in 1 and 4.954 ꢀ in 2) and
“b” (12.423 ꢀ in 1 and 12.899 ꢀ in 2)
increased slightly, “c” (19.626 ꢀ in
1 and 16.128 ꢀ in 2) decreased consid-
erably leading to a reduction in cell
volume and
a concomitant 11.7%
increase in density. A comparison of
the crystal structures of the monomer
1 and the polymer 2 revealed that major
positional changes, after polymeri-
zation, are in the “c” direction (see
Supporting Information). This change
could be due to the formation of
covalent linkages at the expense of
Figure 3. Comparison of the 1H NMR and 13C NMR spectra of monomer 1 with polymer 2.
that the crystals of 1 undergo topochemical polymerization
and the degree of polymerization increases with time and
temperature.
noncovalent interactions along this direction.
4
Sugar units in their normal C1 conformation are con-
nected through the 1,4-triazolyl moiety along the “c”
direction forming polymeric chains. The polymer chain
adopts a right-handed helical conformation in the crystals in
which each sugar unit is cork-screwed 1808 relative to its
neighbor. Though the crystal structure of galactan, the natural
polymer of d-galactose, has not been reported to date,
modeling studies predicted a right-handed helical structure
for b(1,4)-d-galactan.[20] The one dimensional zigzag hydro-
gen-bonded arrangement along “a” direction, as observed in
monomer 1, is also conserved in the polymer 2. While in the
monomer 1, two hydroxy groups are involved in forming two
The progress of the reaction was monitored by IR and
1H NMR spectroscopy. While the IR spectrum of the
monomer 1 showed a sharp signal at 2130 cmÀ1 from the
azide stretching, the azide signal has almost disappeared in
the IR spectrum of a sample kept at 908C for 12 h or 1008C
for 1 h (see Supporting Information). The 1H NMR spectra of
the heated sample also showed the absence of the signals
arising from monomer 1 (e.g. H-1 at d = 4.41 ppm) and the
presence of the triazolyl proton signal (d = 8.22 ppm). The
1H NMR and 13C NMR spectra of the polymer were very
clear, with distinct signals for each proton and carbon atom of
the repeating unit, suggestive of the formation of higher
polymers of uniform size (Figure 3). Structural assignment
using various NMR techniques revealed the presence of only
1,4-triazolyl linkages between the sugar units (see Supporting
Information). This regiospecificity is due to the topochemical
control of the polymerization. Note that uncatalyzed thermal
reactions in solution lead to non-selective cycloaddition
forming a heterogeneous mixture of products, but CuI
catalyzed reactions in solution lead to the formation of
a mixture of 1,4-triazolyl-linked cyclic oligomers (see Sup-
porting Information).
À
À
parallel extended hydrogen bonded (O2 H2’···O3 and O3
À
H3’···O2) zigzag chains, only a single hydrogen bond (O3
H3’···O3) between neighboring sugar units of adjacent
polymer chains is involved in the zigzag arrangement in the
polymer 2 (Figure 4). Also, it is interesting to note that both
O2–H2’ and O3–H3’ change their H-bond acceptor partners
after the polymerization. While the O3–H3’ changes its
partner from O2 to O3, the O2–H2’ changes its acceptor
partner from O3 to N3 in the polymer (Figure 5). The gt
conformation of the hydroxymethyl group is maintained in
the polymer too, which allows interchain hydrogen bonds
between O6–H6’ and O5 of a sugar unit in the adjacent chain.
To correlate structure and properties and to aid the design
of better properties, it is necessary to have high-quality solid-
state structures of polymers. However, the structural charac-
terization of both natural and synthetic polysaccharides is
a formidable challenge because of their amorphous nature
and difficulty in their crystallization from a heterogeneous
mixture. Only very few crystal structures of polysaccharides
The products of many topochemical polymerizations are
either amorphous or microcrystalline which does not allow
structural determination through single-crystal X-ray diffrac-
tion (XRD).[18] There are very few examples for which the
structure of polymer could be solved by single-crystal
XRD.[8a,9c,12,19] As the crystal morphology was preserved in
our case, even after polymerization (kept for 5 h at 1008C),
4
ꢀ 2013 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2013, 52, 1 – 6
These are not the final page numbers!