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concentration, and the melting transition can be varied to a limited
extent. The gel does not swell upon addition of further water but
rather some of the terpy diffuses into a supernatant water layer,
transforming the water layer into a gel of different consistency
instead. Metal binding to give both M(1) and M(1)2 complexes
(M = CoIII, CuII) inhibits gel formation, most likely due to the
coordination geometry on the metal which acts as a sterical barrier;
bulky groups at the periphery of the terpy also inhibit gel formation
Fig. 4 XRD structure of Co(1)2(Cl)2 (atoms are drawn at the 50% probability level as does removal of the carboxy group. The XRD structure of the
after anisotropic refinement).
cobalt complex could be solved, which demonstrates that the
octahedral environment around the cobalt centre is not suitable
for efficient p–p stacking of the terpy units. The gels are now under
some representative examples of the SEM pictures obtained.
investigation for further applications in electrochemistry and ion
These seem to be the preferred morphologies for the freshly
transport, because the terpy unit could be used as an electro-
formed terpy gels. Upon ageing for several weeks in air, the
chemically active sensor moiety in gel-loaded electrodes.
morphology of the gels alters significantly, and either columnar
This work was supported by the EPSRC (EP/F009186/1).
structures or formation of micro-crystalline structures were
observed (Fig. 3c and d). The gels obviously rearrange their
structure over time when exposed to moist air.
Notes and references
Since the terpyridine is a versatile ligand for transition metals,
and some further substituted complexes have shown gelation,3b,12
we also investigated whether metal complexation has an influence
on the behaviour of 1 towards hydrogel formation. We studied both
cobalt and copper due to their ease of formation, and the com-
plexes were made in situ. A 0.5 : 1, 1 : 1 and 2 : 1 mixture of metal
chloride to 1 was used for the formation of the complexes, using
either water or DMF as solvent. The formation of the complexes
could be detected using UV-vis spectroscopy, but they remained
largely insoluble in water or DMF, thus gelation was not occurring
with these systems. Similarly, preformed ruthenium or platinum
complexes were not soluble enough under the gelation conditions.
‡ Data were collected on a Bruker Nonius KappaCCD using a Mo
rotating anode generator; standard procedures were followed. The
crystals lost solvent very rapidly and data collection, structure solution
and refinement were very problematical, however the basic structure is
clear. Crystal data for 2011sot0106 (AG/6043/33/F2) C62H72Cl2CoN12O10
,
%
Mr = 1275.15, T = 120(2) K, triclinic, space group P1, a = 8.7683(15), b =
18.903(3), c = 19.765(4) Å, a = 76.568(10), b = 80.430(10), g = 85.719(11)1,
V = 3139.8(10) Å3, rcalc = 1.349 g cmꢀ3, m = 0.426 mmꢀ1, Z = 2, reflections
collected: 16592, independent reflections: 8528 (Rint = 0.0778), GOF =
1.961, final R indices [I > 2s(I)]: R1 = 0.1998, wR2 = 0.4262, R indices
(all data): R1 = 0.2688, wR2 = 0.4543, largest difference peak and
hole = 0.975 and ꢀ0.865 e Åꢀ3
.
1 U. S. Schubert and C. Eschbaumer, Angew. Chem., Int. Ed., 2002, 41,
2893–2926.
2 (a) A. C. Benniston, A. Harriman, C. Pariani and C. A. Sams, J. Phys.
Chem. A, 2007, 111, 8918–8924; (b) P. P. Kumar, G. Premaladha and
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2+
However, we were able to grow single crystals of the Co(1)2
complex from the DMF solution, a complex which was previously
not analysed by single crystal XRD (Fig. 4).‡ The complex forms
a distorted octahedral meridional complex and crystallises as the
di-chloride with six solvent DMF molecules. Both chlorides are
hydrogen bonded to the adjacent carboxylate hydrogens and a 3D
network is supported by C–HꢁꢁꢁCl contacts. The DMF molecules sit
in pockets within the structure. The crystals lost solvent very
rapidly, therefore the rather low quality of the diffraction and the
structure refinement did not allow for further detailed analysis of
the structure. However, the fact that the metallated terpyridines
crystallise rather than forming a gel supports the fact that a planar
structure is essential for gelation and p-stacking plays a central role
in the process.
In summary, the metal ligand 40-para-phenylcarboxy-terpyridine
1 has been shown to form a thermally reversible fluorescent gel
with a water content of up to 99.2%. The gelation is likely due to
efficient p–p stacking of the hydrophobic terpy units, combined
with formation of the sodium induced salt bridge between terpy-
carboxylates and hydrogen bonded networks with the enclosed
water clusters and between the terpy units, as was observed
3 (a) E. J. Cho, I. Y. Jeong, S. J. Lee, W. S. Han, J. K. Kang and
J. H. Jung, Tetrahedron Lett., 2008, 49, 1076–1079; (b) A. Gasnier,
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previously with pyridine systems.13 In their case, intermolecular 12 F. Camerel, R. Ziessel, B. Donnio, C. Bourgogne, D. Guillon,
hydrogen bonding with weak p–p stacking was accounted for
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13 T. H. Kim, J. Seo, S. J. Lee, S. S. Lee, J. Kim and J. H. Jung, Chem.
fluorescence in the gel, which could equally be the case in our
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c
This journal is The Royal Society of Chemistry 2013
Chem. Commun., 2013, 49, 731--733 733