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Soft Chemical Design of Transition-Metal-Oxide/Clay Layered Nanocomposites

Published online by Cambridge University Press:  21 February 2011

Kiyitali Fuda
Affiliation:
Deptment of Materials-process Engineering and Applied Chemistry for environments, Faculty of Engineering and Resource Science, Akita University, Akita 010-8502, Japan, udak@ipc.akita-u.ac.jp
Shuji Narita
Affiliation:
Deptment of Materials-process Engineering and Applied Chemistry for environments, Faculty of Engineering and Resource Science, Akita University, Akita 010-8502, Japan
Shuji Kudo
Affiliation:
Deptment of Materials-process Engineering and Applied Chemistry for environments, Faculty of Engineering and Resource Science, Akita University, Akita 010-8502, Japan
Kenji Murakami
Affiliation:
Deptment of Materials-process Engineering and Applied Chemistry for environments, Faculty of Engineering and Resource Science, Akita University, Akita 010-8502, Japan
Toshiaki Matsunaga
Affiliation:
Deptment of Materials-process Engineering and Applied Chemistry for environments, Faculty of Engineering and Resource Science, Akita University, Akita 010-8502, Japan
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Abstract

Room-temperature synthesis of transition metal ( TM = Co, Ni and Mn ) oxide intercalated clays has been developed, which extends the potentiality of clay based materials for the design of electroactive nanophase. The structure was examined by using powder XRD - one-dimensional Fourier analysis, magnetic susceptibility measurement as well as conventional analytical methods. From the results, it was revealed that the oxidation by using NaClO as the oxidative reagent affords a new expanded layer structure with a basal spacing of about 1.96 nm wherein a conductive TM oxide sheetadjacent to two hydrated sodium ion layers resides in the gallery of the clay. The resultant sodium cobaltate interlayered smectite bears multi-functionality; an apparent bulk conductivity in the order of 10−5 Scm−1 and a cation exchange ability.

Type
Research Article
Copyright
Copyright © Materials Research Society 2000

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References

References And Note

[1] Hwu, S.-J., Chem. Mater. 10, 2846 (1998)Google Scholar
[2] Ohtsuka, K., Suda, M., Tsunoda, M., Ono, M., M. Chem. Mater. 2, 511 (1990)Google Scholar
[3] Yamanaka, S., Brindley, G. W., Clays Clay Miner. 26, 21 (1978)Google Scholar
[4] Brindley, G. W., Kao, C., Clays Clay Miner. 28, 435 (1980)Google Scholar
[5] The analysis was carried out by using the following equations, I001 = A*Lp(θ)*|F001|2 , where Lp(θ) = (1+cos2(2θ))/(sin2(θ)cos(θ)), and A stands for a instrumental constant. The electorn density ρ(z) was calculated by using a equation, ρ(z) = ∑F001cos(2πzl). The signs of Fobs were phased with the calculated ones on the basis of the structure model.Google Scholar
[6] Jansen, Von M. and Hoppe, R., Z. anorg. Allg. Chem. 408, 104 (1974)Google Scholar
[7] Schollhorn, R., Ang. Chemie 19, 983 (1980)Google Scholar
[8] Reimers, J. N., Dahn, J. R., Greendan, J. E., Stager, C. V., Liu, G, Davison, I., and Sacken, U. Von, J. Sol. St. Chem. 102, 542 (1993)Google Scholar
[9] Leroux, F, Guyomard, D., and Piffard, Y., Sol. St. Ionics 80, 299 (1995)Google Scholar