ChemComm
Communication
the separation upon further additions (2.0–4.0 equiv.) of the
base. Furthermore, the H2 and H3 (4H, d 8.00 ppm) protons
ꢀ
ꢀ
from the same ring may not be involved in stacking, as these
hardly exhibited any shift. Moreover, amongst phenolate ring
protons (8H; H5, H6, H7 and H8, d 7.44–6.66 ppm) only H6 and
ꢀ
ꢀ
ꢀ
ꢀ
ꢀ
H8 (o- and p- to phenolate oxygen) displayed an upfield shift
ꢀ
with broad features. This may be due to their involvement in
6
b,7
C–Hꢁ ꢁ ꢁp type interactions.
The concomitant disappearance Fig. 2 (a) DFT-optimized structure of 2 showing the involvement of
the isophthalate ring planes in p–p/cation–p interactions; (b) dynamic
temperature ramp of the loss of tangent (tan d = G /G ) at 5 1C min
showing the phase transition temperature (Tgel) 84 1C for gel.
of signals in the aliphatic region corroborated well with clea-
00
0
ꢀ1
,
vage of the ester linkage (–CH
and –CH , 12H; H10 and H12, d 1.28 ppm) (Fig. S8, ESI†).
2
–, 8H; H9 and H11, d 4.28 ppm
ꢀ
ꢀꢀ
3
ꢀꢀ
ꢀꢀ
Involvement of the H1 in p-stacking was confirmed by a VT
ꢀ
1
H NMR experiment, as it successively exhibited a high field shift Complex viscosity measurements at increasing temperature
(Dd, 0.09) at 55 1C. Thus, the NMR studies undoubtedly demon- supported the phase transition at 80 1C. This shows phase
strated the conversion of esters into a carboxylate moiety (1 - 2) transition via gel–semi sol–solid, which is expected for a mixed
with an appropriate conformation for p-interactions favourable solvent-based inorganic gel, and it indicates formation of a
for aggregation, and consecutively, for gelation.
typical ‘soft-solid’ like gel phase material. This observation is
To firmly validate the significant conformational reorgani- consistent with the VT fluorescence studies. A double logarithmic
zation, DFT optimizations were undertaken on the model plot between the complex viscosity (Z*) and the angular frequency
structures of 1 and 2. The optimized structures clearly showed (o) with a gradient close to ꢀ1 suggests a regular decrease in
substantial geometrical differences from the square planar (1) viscosity with increasing frequency.
0
to the tetrahedral (2) (Fig. S9, ESI†). Distant isophthalate rings
The mechanical strength of the gel was measured using G
2
+
00
in 1 (like the Cu analogue reported in our previous work) are and G as a function of shear stress at 22 1C and a frequency
8
ꢀ1
0
00
close to each other in 2. In doing so, 1 might have undergone of 1 rad s . Over a large range of shear stress, G supersedes G
significant conformational changes, most likely by an enormous by B1 order of magnitude, which clearly indicates a gel phase
ꢀ
+
9
increase (B185 fold) in the dipole moment due to the –COO Na
material. Notably, with a gradual increase in the applied
+
ꢀ
0
00
moiety. Two Na ions are flanked with the –COO moieties of stress, both G and G remained almost invariant and cross
the native isophthalate rings, while the other two are flanked by each other only at a certain yield stress (1.3 Pa), showing non-
ꢀ
+
the –COO of both isophthalate rings. Na ions are also linear properties and indicating mechanical breaking of the gel
involved in significant interactions with the subsequent iso- beyond the yield stress following a phase transition (gel–sol).
phthalate rings, which provide strong evidence of the dominant On the other hand, IGM is mechanically stable for an applied
cation–p interactions (2.13–2.76 Å). The optimized structure of strain up to 1.2% (Fig. S10, ESI†). Frequency sweep measure-
0 00
2
favours p–p stacking interactions involving isophthalate ments showed G and G to be frequency independent in the
+
ꢀ1
0
00
rings, even after involvement of the Na ion in close proximity, frequency region (ꢀ0.2–1.5 rad s ). As G 4 G , this suggests
and thereby supports the downfield shift for the H1 proton. that the IGM behaves as a gel phase material. The gelation
ꢀ
Moreover, it confirms the intermolecular p-interactions that are property was also probed by comparative PXRD patterns for 1
indispensable for gelation due to the position of the fourth Na , and its xerogel. The loss of the peaks due to xerogel established
+
1
0
which is most probably involved in interplanar cation–p interac- its amorphous nature (IGM) (Fig. S11, ESI†). Based on the
tions. On the contrary, phenolate rings are distant enough that they above results, it is concluded that saponification is the key
can only get involved in stabilization of the supramolecular net- observable step that induces significant conformational change
work (gel matrix) via weak C–Hꢁꢁꢁp interactions for aggregation, in 1 by the in situ conversion of the ester into carboxylate,
and therefore support unusual chemical shifts for the phenolate thereby increasing the p-interactions by manifolds to create a
1
1
ring protons (H6 and H8). Thus, the conclusions drawn from the true phase gel material (IGM) (Fig. S14, ESI†).
spectral studies are consistent with the observations elicited
ꢀ
ꢀ
In summary, through this work the applicability of the
from the DFT-optimized structures (Fig. 2a). The inability of saponification process to trigger gelation in a Zn(II) complex
2
+
2+
2+
Cu , Ni and Co analogues to form a gel can also be explained has been demonstrated. Gelation is accompanied by substan-
by performing DFT calculations (Fig. S9, ESI†). tial conformational changes encompassing gel-phase oriented
To exclude the artefacts of the gel phase material, freshly p-stacking/cation–p interactions. This has been thoroughly
1
prepared IGM was directly subjected to rheological studies. At demonstrated by various spectral (UV/vis, fluorescence, H NMR)
0
fixed concentrations of IGM (1.4%, w/v), the storage (G ) and and DFT studies, and the true gel phase was also affirmed by
00
loss modulus (G ) were measured in the temperature range rheological investigations. Therefore, through this work a novel
0
00
2
2–100 1C, and it was observed that G 4 G up to 84 1C. The gel methodology based on saponification-triggered gelation for
started to deform at 70 1C and ended at 84 1C, where both inorganic complexes has been established.
0
00
the moduli meet each other (G = G ), suggesting a phase
The authors thank DST and UGC, New Delhi, India for
transformation. A sharp change in the loss tangent value providing the Fluorescence Spectrometer through the scheme
00
0
5b
(
tan d = G /G ) at 84 1C specifies Tgel for IGM (Fig. 2b).
SR/S1/IC-25/2011 (DSP), and Senior Research Fellowship through
10088 | Chem. Commun., 2014, 50, 10086--10089
This journal is ©The Royal Society of Chemistry 2014