Phosphoric Acid Loaded Azo ( N N ) Based Covalent Organic Framework For Proton Conduction
Phosphoric Acid Loaded Azo ( N N ) Based Covalent Organic Framework For Proton Conduction
Phosphoric Acid Loaded Azo ( N N ) Based Covalent Organic Framework For Proton Conduction
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© 2014 American Chemical Society 6570 dx.doi.org/10.1021/ja502212v | J. Am. Chem. Soc. 2014, 136, 6570−6573
Journal of the American Chemical Society Communication
counterpart, i.e. stilbene functionalized COF (Tp-Stb) which peaks at 5.5°, 6.4°, 8.4°, and 27° (001 plane). The π−π stacking
shows less stability, crystallinity, porosity, and much less proton distance between COF layers was calculated to be 3.3 Å from the
conductivity than Tp-Azo because of the nonavailability of an d spacing between 001 planes. On the other hand, Tp-Stb
anchoring site. exhibits an intense peak at 2θ = 3.2° followed by a broad peak at
The syntheses of Tp-Azo and Tp-Stb were done by reacting 5.5°. A possible 2D model was built with an eclipsed structure in
Tp (63 mg, 0.3 mmol) with Azo (96 mg, 0.45 mmol) or Stb (128 the hexagonal space group (P6/m) and a staggered structure in
mg, 0.45 mmol) using (1:1) dimethylacetamide and o-dichloro- the P1 space group, by using the software Crystal 09.10 The
benzene as solvent (3 mL) (Figure 1). The reactants were first experimental PXRD pattern matches well with the simulated
pattern of the eclipsed stacking model (Figures S1 and S3,
Supporting Information (SI)). In order to find out the unit cell
parameters, Pawley refinements were done for both of the COFs.
The unit cell value was found to be (a = b = 31.5 Å, c = 3.3 Å) for
Tp-Azo and (a = b = 30.500 Å, c = 3.49 Å) for Tp-Stb. The
intensity ratio of the first and second peak in the eclipsed form
matches with the PXRD of Tp-Stb. The energy calculation of
both eclipsed and staggered forms of Tp-Stb also suggests an
eclipsed stacking model with lower energy (Section S-3, SI).
The FT-IR spectra of Tp-Azo and Tp-Stb indicate the total
consumption of starting materials due to the disappearance of the
N−H stretching bands (3100−3300 cm−1) of Azo or Stb and the
carbonyl stretching bands (1639 cm−1) of Tp (Figure 2b). The
strong peak at 1578 cm−1 arises due to the CC stretching in the
keto-form similar to the FT-IR spectrum of the reference
compound 2,4,6-tris((phenyldiazenyl)phenylamino-
methylene)cyclohexane-1,3,5-trione. Most of the FT-IR peaks
of Tp-Azo and Tp-Stb match well with those of the reference
compound (Figure 2b). The CO peaks (1619 cm−1) of Tp-
Azo and Tp-Stb get merged with the CC stretching band
(1582 cm−1). The isolation of Tp-Azo and Tp-Stb as the keto-
form was confirmed by 13C CP-MAS solid state NMR. Both
COFs show carbonyl (CO) carbon signals at δ = 181 and 186
ppm for Tp-Azo and Tp-Stb respectively. In the starting
material, the trialdehyde carbonyl (CO) carbon resonates at a
downfield position around δ = 192 ppm. The absence of a peak at
δ = 192 ppm in the 13C CP-NMR spectrum also indicates the
total consumption of the starting materials (Figures 2c and S-8,
Figure 1. (a) Crystal structure of 4-[(E)-phenyl-diazenyl]anilinium
dihydrogen phosphate.9a (b) Schematic of Tp-Azo and Tp-Stb SI). To investigate the protonation of the azo bond by
synthesis. phosphoric acid in PA@Tp-Azo, we have done 31P CP-NMR,
which shows two distinct peaks at δ −1.31 ppm and δ −14.3
ppm. The 31P resonance peak at δ −1.31 ppm is attributed to the
dispersed by ultrasonication for 10 min and then degassed undissociated H3PO4 and the shoulder at δ −14.3 ppm
through three freeze−pump−thaw cycles. The tubes were then corresponds to the H2PO4− anion, which indicates the
vacuum sealed and placed in an isotherm oven for 3 days at 120 protonation of the azo bond. However, in PA@Tp-Stb, only a
°C. Finally, the material was filtered out and washed with dry single intense peak at δ −0.88 ppm, corresponding to
acetone and dried under vacuum at 150 °C for 12 h. The PXRD undissociated H3PO4, has been observed and the peak at δ
patterns of Tp-Azo indicate an intense peak at 2θ = 3.2°, which −14.3 ppm was absent. This explains the absence of the H2PO4−
corresponds to 100 plane reflections (Figure 2a), with minor anion due to the lack of protonation sites in Tp-Stb (Figure 3b).
Figure 2. (a) Observed PXRD patterns of Tp-Azo (blue) and Tp-Stb (green) compared with simulated eclipsed patterns. (b) FT-IR spectra of Tp-Azo
and Tp-Stb compared with starting material Tp, Azo, and Stb. (c) 13C NMR comparison of Tp-Azo (blue), Tp-Stb (green) against the reference
compound Tp-Azo monomer = 2,4,6-tris(((4-((E)-phenyldiazenyl)phenyl)amino)methylene)cyclohexane-1,3,5-trione (red).
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Communication
under 98% relative humidity (RH) (Section S-13, SI). The AUTHOR INFORMATION
proton conductivity of PA@Tp-Azo is lower than that of its Corresponding Author
MOF counterparts, i.e. ferrous oxalate dihydrate5e (1.3 × 10−3 S r.banerjee@ncl.res.in
cm −1 at 298 K, 98% RH) and 1,2,4-triazole loaded β-PCMOF2 Author Contributions
(5 × 10−4 S cm−1 at 423 K, 20% RH) (full comparison in Table †
S.C. and T.K. contributed equally.
S3 in SI). Surprisingly, PA@Tp-Stb shows almost zero proton
conductivity in anhydrous conditions, while exhibiting a poor Notes
proton conductivity value of 2.3 × 10−5 S cm−1 at 332 K under The authors declare no competing financial interest.
98% RH. Notably, PA@Tp-Azo exhibited an activation energy
value of 0.11 eV (Figure 4e), which is much lower than that of
Nafion (0.22 eV) and its MOF counterparts (Table S3, SI)
■ ACKNOWLEDGMENTS
S.C. and T.K. acknowledge UGC and CSIR (New Delhi, India)
operating under humid conditions. Clearly, PA@Tp-Azo and for JRF and SRF. R.B. acknowledges [CSC0122 and CSC0102]
PA@Tp-Stb show distinct proton conductivity behavior under and DST (SB/SI/IC-32/2013) for funding. We acknowledge Dr.
similar conditions, although they are treated with the same T. G. Ajithkumar, Dr. K. Sreekumar, and Dr. C. Ramesh for
NMR, Proton Conduction, and PXRD facilities.
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amount of H3PO4. Nevertheless, Tp-Azo exhibits a distinct color
change (red to black) upon H3PO4 treatment, while the color of
Tp-Stb remains almost unchanged (gray). The UV−vis spectra REFERENCES
of the H3PO4 treated Tp-Azo monomer are red-shifted from 380 (1) (a) Côté, A. P.; Benin, A. I.; Ockwig, N. W.; Matzger, A. J.;
to 496 nm due to the protonation of the azo bond (Figures S25 O’Keeffe, M.; Yaghi, O. M. Science 2005, 310, 1166. (b) Feng, X.; Ding,
and S26). However, the −NH− and the −CC− groups remain X.; Jiang, D. Chem. Soc. Rev. 2012, 41, 6010. (c) Colson, J. W.; Dichtel,
W. R. Nat. Chem. 2013, 5, 453.
unaffected after acid treatment, which can be proved from the
(2) (a) Janiak, C. Dalton Trans. 2003, 2781. (b) O’Keeffe, M.; Yaghi, O.
intact UV−vis spectra of 2,4,6-tris(([1,1′-biphenyl]-4-ylamino)- M. Chem. Rev. 2012, 112, 675. (c) Zhou, H. C.; Long, J. R.; Yaghi, O. M.
methylene)cyclohexane-1,3,5-trione (monomer of TpBD) and Chem. Rev. 2012, 112, 673. (d) Furukawa, H.; Cordova, K. E.; O’Keeffe,
stillbene. These observations hint at the interaction between the M.; Yaghi, O. M. Science 2013, 341, 6149.
proton responsive azo group and H3PO4, which is the governing (3) (a) Han, S. S.; Furukawa, H.; Yaghi, O. M.; Goddard, W. A. J. Am.
factor for the high proton conductivity value of PA@Tp-Azo in Chem. Soc. 2008, 130, 11580. (b) Furukawa, H.; Yaghi, O. M. J. Am.
both humid and anhydrous conditions, a mechanism absent in Chem. Soc. 2009, 131, 8875. (c) Rabbani, M. G.; Sekizkardes, A. K.;
PA@Tp-Stb. We anticipate that the loaded H3PO4 along with Kahveci, Z.; Reich, T. E.; Ding, R.; El-Kaderi, H. M. Chem.Eur. J.
adsorbed water molecules get H-bonded with the protonated azo 2013, 19, 3324. (d) Wan, S.; Guo, J.; Kim, J.; Ihee, H.; Jiang, D. Angew.
groups stacked along the crystallographic a axis, which conduct Chem., Int. Ed. 2008, 120, 8958. (e) Dogru, M.; Handloser, M.; Auras, F.;
Kunz, T.; Medina, D.; Hartschuh, A.; Knochel, P.; Bein, T. Angew. Chem.
the proton through the framework.
2013, 52, 2920. (f) Gopalakrishnan, D.; Dichtel, W. R. J. Am. Chem. Soc.
In summary, we for the first time have reported azo and alkene 2013, 135, 8357.
functionalized COFs (Tp-Azo and Tp-Stb) as proton (4) (a) Mauritz, K. A.; Moore, R. B. Chem. Rev. 2004, 104, 4535.
conducting materials. Exceptional chemical stability, low density, (b) Hickner, M.; Ghassemi, H.; Kim, Y. S.; Einsla, B. R.; McGrath, J. E.
and high thermal stability make them advantageous over their Chem. Rev. 2004, 104, 4587. (c) Paddison, S. J. Annu. Rev. Mater. Res.
MOF counterparts. We have demonstrated a simple impregna- 2003, 33, 289.
tion strategy to load mineral acid viz. H3PO4 inside the (5) (a) Ponomareva, V. G.; Kovalenko, K. A.; Chupakhin, A. P.;
framework. Interestingly, after the acid treated samples are Dybtsev, D. N.; Shutova, E. S.; Fedin, V. P. J. Am. Chem. Soc. 2012, 134,
washed, the COFs retain their crystallinity, porosity, and stability, 15640. (b) Bureekaew, S.; Horike, S.; Higuchi, M.; Mizuno, M.;
which make them attractive for proton conduction applications. Kawamura, T.; Tanaka, D.; Yanai, N.; Kitagawa, S. Nat. Mater. 2009, 8,
831. (c) Hurd, J. A.; Vaidhyanathan, R.; Thangadurai, V.; Ratcliffe, C. I.;
While the parent COFs exhibit negligible conductivity, PA@Tp-
Moudra-kovski, I. M.; Shimizu, G. K. H. Nat. Chem. 2009, 1, 705.
Azo shows decent proton conductivity values under both (d) Yoon, M.; Suh, K.; Kim, H.; Kim, Y.; Selvapalam, N.; Kim, K. Angew.
hydrous and anhydrous conditions. PA@Tp-Stb, on the other Chem., Int. Ed. 2011, 50, 7870. (e) Yamada, T.; Sadakiyo, M.; Kitagawa,
hand, exhibits poor proton conductivity and, that too, only under H. J. Am. Chem. Soc. 2009, 131, 3144.
hydrous conditions. Thus, minute changes in functionality lead (6) (a) Lanni, L. M.; Tilford, R. W.; Bharathy, M.; Lavigne, J. J. J. Am.
to a drastic change in proton conducting ability, which establishes Chem. Soc. 2011, 130, 11872.
the crucial role of the proton responsive azo group in facilitating (7) (a) Kandambeth, S.; Mallick, A.; Lukose, B.; Mane, V. M.; Heine,
proton conduction pathways. Although 2D COFs lack long- T.; Banerjee, R. J. Am. Chem. Soc. 2012, 134, 19524. (b) Biswal, B. P.;
range ordering in bulk solid and generate a grain boundary (like Chandra, S.; Kandambeth, S.; Lukose, B.; Mane, V. M.; Heine, T.;
MOFs) which may decrease proton conductivity, 3D COFs11 Banerjee, R. J. Am. Chem. Soc. 2013, 135, 5328. (c) Chandra, S.;
Kandambeth, S.; Biswal, B. P.; Lukose, B.; Kunjir, S. M.; Chaudhary, M.;
with the azo group (−NN−) acting as a phosphoric acid
Babarao, R.; Heine, T.; Banerjee, R. J. Am. Chem. Soc. 2013, 135, 17853.
anchoring site could prove advantageous in the long run. In (8) Asensio, J. A.; Sanchez, E. M.; Gomez-Romero, P. Chem. Soc. Rev.
addition, the membrane compatibility of COFs may be beneficial 2010, 39, 3210.
toward the preparation of COF−polymer composites, an (9) (a) Halasz, I.; Lukic, K.; Vancik, H. Acta Crystallogr. 2007, C63,
ongoing effort in our laboratory. We believe that our findings o61. (b) Sanchez, A. M.; Barra, M.; de Rossi, R. H. J. Org. Chem. 1999,
will encourage further work in COF based functional proton 64, 1604.
conducting materials in the near future. (10) Dovesi, R.; Saunders, V. R.; Roetti, C.; Orlando, R.;
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ZicovichWilson, C. M.; Pascale, F.; Civalleri, B.; Doll, K.; Harrison, N.
ASSOCIATED CONTENT M.; Bush, I. J.; Arco, P. D.; Llunell, M. Crystal 1.0.2 ed.
(11) Beaudoin, D.; Maris, T.; Wuest, J. D. Nat. Chem. 2013, 5, 830.
*
S Supporting Information
Synthetic procedures, PXRD, 13C solid state NMR, TGA, UV,
crystallographic data (CIF). This material is available free of
charge via the Internet at http://pubs.acs.org.
6573 dx.doi.org/10.1021/ja502212v | J. Am. Chem. Soc. 2014, 136, 6570−6573