B368 Journal of The Electrochemical Society, 159 (4) B368-B370 (2012) 0013-4651/2012/159(4)/B368/3/$28.00 © The Electrochemical Society Effect of Mg/Al Ratio on Hydroxide Ion Conductivity for Mg–Al Layered Double Hydroxide and Application to Direct Ethanol Fuel Cells Kiyoharu Tadanaga, z Yoshihiro Furukawa, Akitoshi Hayashi, ∗ and Masahiro Tatsumisago Department of Applied Chemistry, Graduate School of Engineering, Osaka Prefecture University, Naka-ku, Sakai, Osaka 599-8531, Japan Mg–Al layered double hydroxides (LDHs) intercalated with carbonate anions were prepared by the co-precipitation process with Mg/Al = 2, 3 and 4, and the effect of Mg/Al ratio on the ionic conductivity was examined. It is shown that the Mg/Al ratio influences ionic conductivities of Mg–Al CO3 2− LDH. The conductivity of Mg-Al CO3 2− LDH with Mg/Al = 2 and 3 exhibited almost the same ionic conductivity of about 1 × 10−3 S cm−1 at room temperature under 80% relative humidity, while that of LDH with Mg/Al = 4 was lower by one order of magnitude. Thermal analyses showed that Mg-Al CO3 2− LDH with Mg/Al = 2 or 3 keeps interlayer water molecules at higher temperatures compared with Mg/Al = 4, suggesting that the interlayer water molecules are strongly held in the interlayer. The strongly held interlayer water molecules are assumed to contribute the high ionic conductivity in Mg-Al CO3 2− LDH with Mg/Al = 2 and 3. The alkaline type direct ethanol fuel cells using Mg/Al CO3 2− LDHs as hydroxide conducting electrolyte were confirmed to operate, and larger power was obtained in Mg-Al CO3 2− LDH with smaller Mg/Al ratio. © 2012 The Electrochemical Society. [DOI: 10.1149/2.007204jes] All rights reserved. Manuscript submitted March 31, 2011; revised manuscript received November 22, 2011. Published January 18, 2012. Layered double hydroxides (LDHs) are anionic clays consisting of positively charged metal hydroxide layers with anions located in the interlayer for charge compensation of the cationic layers. The chemical formula for LDHs is [MII 1−x MIII x (OH)2 ]x+ (An− )x/n · mH2 O, where MII is a divalent metal cation, MIII is a trivalent cation, and An− is an anion. Because of their potential application as anion exchangers, catalysts, electrochemical sensors and bio-active materials, LDHs have received increasing attention in recent years.1–4 The layered structure in LDHs incorporates anions and water molecules in the interlayer, and thus, they can be interesting materials for use as solid electrolytes. Nevertheless, few reports have described investigations of ionic conductivities of LDHs.5, 6 In fuel cells, LDHs have been used only as fillers for proton conductive membranes,7, 8 or effects of the addition of LDHs to the catalyst layer of alkaline-type direct alcohol fuel cells have been reported.9, 10 Very recently, we examined the ionic conductivity for Mg-Al layered double hydroxides (LDHs) intercalated with several inorganic anions11 reporting that they have high ionic conductivity under 80% relative humidity. We also clarified that Mg-Al LDH intercalated with CO3 2− is a hydroxide ion conductor under the humidified condition by water vapor concentration cell measurements, and showed that Mg-Al CO3 2− LDH functions as an electrolyte for alkaline type direct ethanol fuel cells (DEFCs).12 In LDHs, trivalent cations replace divalent cation, and the replacement of divalent cations with trivalent cations generates a positive charge on the hydroxide layers of LDH. Thus, the degree of replacement affects the amount of interlayer anions, and may also affect the ionic conductivity. In the present study, effects of Mg/Al ratio on the ionic conductivity of the Mg–Al CO3 2− LDHs were examined. Performance of DEFCs using the Mg–Al CO3 2− LDHs as electrolyte was also examined. Experimental Using the co-precipitation method with controlled pH, Mg– Al CO3 2− LDHs were prepared.13 A mixed solution containing Mg(NO3 )2 · 6H2 O and Al(NO3 )3 · 9H2 O with Mg2+ /Al3+ = 2, 3 and 4 was added dropwise into 0.3 M Na2 CO3 solution with stirring at 80◦ C. The pH of the mixture was adjusted to 10 by the addition of 2 M NaOH solution and the reaction mixture was aged at 80◦ C for 17 h. The resulting white precipitates were filtrated, washed with distilled water, and dried at 80◦ C. The precipitates consisted of ag∗ Electrochemical Society Active Member. z E-mail: [email protected] gregated particles with a size of a few micrometer, having a primary particle diameter of from several tens to a few hundreds nanometers. X-ray diffraction (XRD) measurements (CuKα) were performed to identify crystalline phases using an XRD diffractometer (Shimazu XRD 6000). Differential thermal analysis and thermogravimetry (DTA-TG) were carried out using a thermal analyzer (Rigaku Termoplus 8120), with a hearting rate of 10◦ C min−1 in N2 . Electrical conductivities of the pellets obtained by cold pressing under a pressure of 360 MPa were measured: the diameters and thickness of the pellets were 10 mm and about 0.5 mm, respectively, and the estimated relative density of the pellet was more than 90%. Gold was evaporated on both sides of the pellets as the electrodes. The conductivity of the pellets was determined from impedance data obtained using an impedance analyzer (Solartron 1260; Solartron Analytical) at frequencies of 1 Hz – 8 × 106 Hz. Performance of DEFCs was examined as described previously.12 A passive-type direct ethanol fuel cell was fabricated using pelletized Mg-Al CO3 2− LDH powder as electrolyte (thickness of the pellet was about 0.3 mm). The anode and cathode electrodes with non-Pt catalysts (HypermecTM ; ACTA S.p.A.) were used, where Ni-Co-based alloy on carbon powder is used for the anode and Fe-Co-based alloy on carbon powder is used for the cathode.14 The cathode and anode backing layers were nickel form and carbon cloth, respectively. The pelletized Mg-Al CO3 2− LDH was sandwiched with the two electrodes and the gold-plated current collectors that were attached with cell fixtures. An aqueous solution of ethanol and potassium hydroxide (10wt %EtOH10wt %KOH) was used as fuel. The volume of the anode compartment was ca. 25 cm3 , and the cathode was exposed to air. The active area of the cell was about 0.4 cm2 . Polarization performances were measured using a potentiostat and galvanostat (Autolab, PGSTAT30) at R.T. Results and Discussion Figure 1 shows the XRD patterns of LDH with Mg/Al = 4, 3 and 2. The basal spacing calculated using those peaks is 0.804, 0.780, and 0.750 nm for Mg/Al = 4, 3, and 2, respectively. The basal spacing decreases with a decrease in Mg/Al ratio from 4 to 2. The basal spacing should be affected by the interaction between inorganic layers. As mentioned above, in LDH, the replacement of divalent cations with trivalent cations generates a positive charge on the hydroxide layers of LDH. Decrease in the Mg/Al ratio means the increase in the amount of substitution of Mg2+ with Al3+ and also the increase in charge of layer. Therefore, the interaction between hydroxide layers is considered to become strong and the basal spacing between layers decreased. Downloaded on 2016-05-12 to IP 130.203.136.75 address. Redistribution subject to ECS terms of use (see ecsdl.org/site/terms_use) unless CC License in place (see abstract). Journal of The Electrochemical Society, 159 (4) B368-B370 (2012) B369 Au / LDH / Au (0 0 3) (0 0 6) 10 Mg/Al = 4 -2 Mg/Al = 3 Conductivity / S cm-1 Intensity / arb.unit d = 0.804nm (0 0 3) (0 0 6) Mg/Al = 3 d = 0.780nm 10 -3 10 -4 10 -5 (0 0 3) (0 0 6) 10 Mg/Al = 2 Mg/Al = 4 2.8 2.9 Mg/Al = 2 d = 0.750nm 20 30 40 2 /deg. (CuK ) 80 %R.H. 3 3.1 3.2 1000/T / K -1 3.3 Figure 3. Temperature dependence of the conductivities for Mg-Al CO3 2− LDH with Mg/Al = 2, 3 and 4. 50 Figure 1. XRD patterns of Mg-Al CO3 2− LDH with Mg/Al = 2, 3 and 4. The DTA-TG curves of Mg-Al CO3 2− LDH with Mg/Al = 4, 3 and 2 are presented in Fig. 2. The weight loss at temperatures between room temperature and 250◦ C can be assigned to the loss of interlayer water in LDH, and the weight loss at higher temperature is assigned to the elimination of H2 O from OH groups in the inorganic layer and CO2 from CO3 2− ions.15 The endothermic peak in the DTA curve at around 200◦ C is shifted to higher temperature side with decreasing Mg/Al ratio. Since the charge density of a hydroxide layer becomes large as Mg/Al becomes small, the interaction between the hydroxide layer and interlayer water molecules should become strong. Thus, Mg-Al CO3 2− LDH with Mg/Al = 2, or 3 keeps the interlayer water molecules at higher temperatures compared with Mg/Al = 4. Temperature dependence of the conductivities for Mg-Al CO3 2− LDH with Mg/Al = 4, 3 and 2, at 80% of the relatives humidity is shown in Fig. 3. The ionic conductivity of Mg-Al CO3 2− LDH with Mg/Al = 2 and 3 is about 10−3 S cm−1 , while that of Mg-Al CO3 2− LDH with Mg/Al = 4 is lower than 10−4 S cm−1 , at room temperature. Moreover, the activation energy of ionic conduction decreases with a decrease in Mg/Al ratio. As shown in Fig. 2, interlayer water molecules are strongly held in Mg-Al CO3 2− LDH with smaller Mg/Al ratio. Because the interlayer molecules can contribute the retention of adsorbed water under humidified conditions, the interlayer molecules are assumed to play an important role in ionic conduction in Mg-Al CO3 2− LDH. Thus, the water molecules strongly held in the layer must contribute the high ionic conductivity and low activation energy in Mg-Al LDH with Mg/Al = 2, and rather low ionic conductivity of LDH with Mg/Al = 4. Although Mg-Al LDHs are known as an anion exchanger, Mg-Al LDH intercalated with CO3 2− is very stable against anion exchange, and thus the ion conducting species is not CO3 2− . As reported previously, Mg-Al CO3 2− LDH with Mg/Al = 3 is confirmed to be a hydroxide ion conductor under the humidified condition. The water vapor concentration cell measurements for Mg-Al CO3 2− LDH Mg/Al = 2 and 4 revealed that these LDHs are also hydroxide ion conductor. Figure 4 shows the cell voltage and power density versus current density for a passive-type DEFC with Mg-Al CO3 2− LDH with Mg/Al = 2, 3 and 4, as an electrolyte and non-platinum catalysts, at room temperature. The cells work as a DEFC; the larger current density is observed at smaller Mg/Al ratio. The maximum power density of about 48 mW cm−2 is obtained for the cell with Mg/Al = 2, which is comparable to that of an active-type DEFC using those non-platinum Mg/Al=2 Mg/Al=3 1 Mg/Al=4 50 0.8 40 0.6 30 0.4 20 -20 0.2 10 -40 0 Mg/Al = 2 20 0 100 200 300 400 500 Figure 2. DTA-TG curves of Mg-Al CO3 2− LDH with Mg/Al = 2, 3 and 4. Cell voltage / V 40 0 50 100 150 200 250 Current density / mA cm-2 Power density / mW cm -2 Mg/Al = 3 Mg/Al = 4 0 300 Figure 4. Performances of the DEFCs using Mg-Al CO3 2− LDH with Mg/Al = 2, 3 and 4 as the electrolyte at room temperature. An aqueous solution of 10wt %EtOH-10wt %KOH was used as fuel. Downloaded on 2016-05-12 to IP 130.203.136.75 address. Redistribution subject to ECS terms of use (see ecsdl.org/site/terms_use) unless CC License in place (see abstract). B370 Journal of The Electrochemical Society, 159 (4) B368-B370 (2012) ences ionic conductivities of Mg–Al CO3 2− LDH. The conductivity of Mg-Al CO3 2− LDH with Mg/Al = 2 and 3 exhibited almost the same ionic conductivity of about 1 × 10−3 S cm−1 at room temperature under 80% relative humidity, while that of LDH with Mg/Al = 4 was lower by one order of magnitude. Thermal analyses showed that MgAl CO3 2− LDH with Mg/Al = 2 or 3 keeps interlayer water molecules at higher temperatures compared with Mg/Al = 4, suggesting that the interlayer water molecules are strongly held in the interlayer. The strongly held interlayer water molecules are assumed to contribute the high ionic conductivity in Mg-Al CO3 2− LDH with Mg/Al = 2 and 3. The alkaline type DEFCs using Mg/Al CO3 2− LDHs as the electrolyte were confirmed to operate, and larger power was obtained in Mg-Al CO3 2− LDH with smaller Mg/Al ratio. -6 Mg/Al=2 Mg/Al=3 Mg/Al=4 Z'' / Ω -4 -2 0 0 1 2 3 Z' / Ω 4 5 Acknowledgments 6 Figure 5. Nyquist plots of the DEFCs using Mg-Al CO3 2− LDH with Mg/Al = 2, 3 and 4, as the electrolyte at room temperature. This work was partly supported by a Grant-in-Aid for Scientific Research from the Ministry of Education, Culture, Sports, Science and Technology of Japan. References 14 catalysts and an anion-exchange membrane or a passive DEFC using Pd/MWCNT anode catalyst and the non-platinum cathode catalyst used in this study with an anion-exchange membrane.16 Nyquist plots of the DEFCs shown in Fig. 4, under the cell operation, are shown in Fig. 5. In the Z vs. Z plot, a few resistance components were observed. The resistance observed in the highest frequency region is attributed to the resistance of the electrolyte. Thus, the Nyquist plots show that the resistance of the electrolyte decreased with a decrease in Mg/Al ratio. In the ionic conductivity measurement under 80% relative humidity, the conductivity of LDHs with Mg/Al = 2 and 3 is almost the same as shown in Fig. 1. However, in the DEFC cell, KOH in the fuel slightly increased the ionic conductivity of the solid electrolyte, and the degree of the increase in conductivity should be higher in Mg/Al = 2. The superior performances at smaller Mg/Al ratio must be caused by the increase in ionic conductivity with a decrease in Mg/Al ratio. Conclusions Effects of Mg/Al ratio on the electrochemical properties of Mg-Al CO3 2− LDH were examined. It is shown that the Mg/Al ratio influ- 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 11. 12. 13. 14. 15. 16. F. Leroux and J. P. Besse, Chem. Mater., 13, 3507 (2001). A. I. Khan and D. O’Hare, J. Mater. Chem., 12, 3191 (2002). X. Guo, F. Zhang, D. G. Evans, and X. Duan, Chem. Commn., 46, 5197 (2010). N. Yamaguchi, T. Nakamura, K. Tadanaga, A. Matsuda, T. Minami, and M. Tatsumisago, Cryst. Growth Des., 6, 1726 (2006). A. de Roy and J. P. Besse, Solid State Ionics, 46, 95 (1991). V. Ducos, A. de Roy, and J. P. Besse, Solid State Ionics, 145, 399 (2001). K. Lee, J.-H. Nam, J. H. Lee, Y. Lee, S. M. Cho, C. H. Jung, H. G. Choi, Y.-Y. Chang, Y.-U. Kwon, and J.-D. Nam, Electrochem. Commun., 7, 113 (2005). Y. Bao, L. Cong, Z.-M Huang, and Z. Weng, J. Mater. Sic., 43, 390 (2008). J. C. Ganley, N. K. Karikari, and D. Raghavan, J. Fuel Cell Sci. Tech., 7, 031019 (2010). K. Miyazaki, T. Abe, K. Nishio, H. Nakanishi, and Z. Ogumi, J. Power Sources, 195, 6500 (2010). Y. Furukawa, K. Tadanaga, A. Hayashi, and M. Tatsumisago, Solid State Ionics, 192, 185 (2011). K. Tadanaga, Y. Furukawa, A. Hayashi, and M. Tatsumisago, Adv. Mater., 22, 4401 (2010). F. Prinetto, G. Ghiotti, P. Graffin, and D. Tichit, Micropor. Mesopor. Mater., 39, 229 (2000). Y. S. Li, T. S. Zhao, and Z. X. Liang, J. Power Sources, 187, 387 (2009). W. Yang, Y. Kim, P. K. T. Liu, M. Sahimi, and T. T. Tsotsis, Chem. Eng. Sci., 57, 2945 (2002). V. Bambagioni, C. Bianchini, A. Marchionni, J. Filippi, F. Vizza, J. Teddy, P. Serp, and M. Zhiani, J. Power Sources, 190, 241 (2009). Downloaded on 2016-05-12 to IP 130.203.136.75 address. Redistribution subject to ECS terms of use (see ecsdl.org/site/terms_use) unless CC License in place (see abstract).
© Copyright 2026 Paperzz