Chromium substituted liSn2P3O12 solid electrolyte

This study was focused on enhancing the conductivity of lithium tin phosphate, LiSn2P3O12 by partially substituting Sn4+ ions with Cr3+ ions to obtain system with general formula Li1+xCrxSn2-xP3O12. Li1+xCrxSn2-xP3O12 powders with x = 0.2, 0.4, 0.6 and 0.8 were prepared by mechanochemical milling me...

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Published in:International Journal of Electrochemical Science
Main Author: Norhaniza R.; Subban R.H.Y.; Mohamed N.S.; Ahmad A.
Format: Article
Language:English
Published: 2012
Online Access:https://www.scopus.com/inward/record.uri?eid=2-s2.0-84872835334&partnerID=40&md5=64fc0172c6b463c7f08210d18bec5317
id 2-s2.0-84872835334
spelling 2-s2.0-84872835334
Norhaniza R.; Subban R.H.Y.; Mohamed N.S.; Ahmad A.
Chromium substituted liSn2P3O12 solid electrolyte
2012
International Journal of Electrochemical Science
7
10

https://www.scopus.com/inward/record.uri?eid=2-s2.0-84872835334&partnerID=40&md5=64fc0172c6b463c7f08210d18bec5317
This study was focused on enhancing the conductivity of lithium tin phosphate, LiSn2P3O12 by partially substituting Sn4+ ions with Cr3+ ions to obtain system with general formula Li1+xCrxSn2-xP3O12. Li1+xCrxSn2-xP3O12 powders with x = 0.2, 0.4, 0.6 and 0.8 were prepared by mechanochemical milling method. X-ray diffraction analysis indicated that all samples consisted of triclinic crystalline LiSn2P3O12 structure. Energy Dispersive X-ray analysis suggested that Cr3+ was successfully substituted into the LiSn2P3O12 crystalline structure. Impedance analysis showed an increase in conductivity with increase in x. The enhancement in bulk conductivity was due to increase in number and polarisability of Li+ ions and crystallinity. The increase in grain boundary conductivity was ascribed to enhancement in Li+ migration as a result of increase in contact between grains. The conductivity versus the reciprocal of temperature plots showed a sudden change in conductivity at 393 K for the sample with x = 0.2 and 373 K for the sample with x = 0.4, 0.6 and 0.8. This was attributed to a structure transitionphenomenon. All samples showed Arrhenian behaviour.© 2012 by ESG.

14523981
English
Article

author Norhaniza R.; Subban R.H.Y.; Mohamed N.S.; Ahmad A.
spellingShingle Norhaniza R.; Subban R.H.Y.; Mohamed N.S.; Ahmad A.
Chromium substituted liSn2P3O12 solid electrolyte
author_facet Norhaniza R.; Subban R.H.Y.; Mohamed N.S.; Ahmad A.
author_sort Norhaniza R.; Subban R.H.Y.; Mohamed N.S.; Ahmad A.
title Chromium substituted liSn2P3O12 solid electrolyte
title_short Chromium substituted liSn2P3O12 solid electrolyte
title_full Chromium substituted liSn2P3O12 solid electrolyte
title_fullStr Chromium substituted liSn2P3O12 solid electrolyte
title_full_unstemmed Chromium substituted liSn2P3O12 solid electrolyte
title_sort Chromium substituted liSn2P3O12 solid electrolyte
publishDate 2012
container_title International Journal of Electrochemical Science
container_volume 7
container_issue 10
doi_str_mv
url https://www.scopus.com/inward/record.uri?eid=2-s2.0-84872835334&partnerID=40&md5=64fc0172c6b463c7f08210d18bec5317
description This study was focused on enhancing the conductivity of lithium tin phosphate, LiSn2P3O12 by partially substituting Sn4+ ions with Cr3+ ions to obtain system with general formula Li1+xCrxSn2-xP3O12. Li1+xCrxSn2-xP3O12 powders with x = 0.2, 0.4, 0.6 and 0.8 were prepared by mechanochemical milling method. X-ray diffraction analysis indicated that all samples consisted of triclinic crystalline LiSn2P3O12 structure. Energy Dispersive X-ray analysis suggested that Cr3+ was successfully substituted into the LiSn2P3O12 crystalline structure. Impedance analysis showed an increase in conductivity with increase in x. The enhancement in bulk conductivity was due to increase in number and polarisability of Li+ ions and crystallinity. The increase in grain boundary conductivity was ascribed to enhancement in Li+ migration as a result of increase in contact between grains. The conductivity versus the reciprocal of temperature plots showed a sudden change in conductivity at 393 K for the sample with x = 0.2 and 373 K for the sample with x = 0.4, 0.6 and 0.8. This was attributed to a structure transitionphenomenon. All samples showed Arrhenian behaviour.© 2012 by ESG.
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language English
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