Fabrication, electrochemical performance, and in situ infrared thermal imaging of Na0.67(Mn0.5Fe0.5)1-xCuxO2 battery cells


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Altın S., Korkusuz K.

International Journal Of Energy Research, vol.11, no.1, pp.1-13, 2021 (SCI-Expanded)

  • Publication Type: Article / Article
  • Volume: 11 Issue: 1
  • Publication Date: 2021
  • Doi Number: 10.1002/er.671110.1002/er.6711
  • Journal Name: International Journal Of Energy Research
  • Journal Indexes: Science Citation Index Expanded (SCI-EXPANDED), Scopus, Academic Search Premier, PASCAL, Aerospace Database, Aquatic Science & Fisheries Abstracts (ASFA), Communication Abstracts, Compendex, Environment Index, INSPEC, Metadex, Pollution Abstracts, Civil Engineering Abstracts
  • Page Numbers: pp.1-13
  • Open Archive Collection: AVESIS Open Access Collection
  • Inonu University Affiliated: Yes

Abstract

Na0.67(Mn0.5Fe0.5)1-xCuxO2 powders (where x = 0, 0.05, 0.1, 0.2, and 0.3) were

produced by quenching at 900C, and the structural features of the powders

were studied in detail. It was found that the undoped and Cu-substituted for

(x ≤ 0.2) powders had no impurity phases in the structure. Furthermore, the

lattice volume calculated by the GSAS-II open-source program decreased with

increasing Cu content, and it is suggested that Cu ions have a 3+ valence state

in the samples. The cycling voltammetry of the cells is very similar to each

other. The constant current charge/discharge cycling measurements were performed

for up to 100 cycles, and the best performance was observed for x = 0.2

Cu substitution in Na0.67(Mn0.5Fe0.5)1-xCuxO2. The best capacity value was

obtained as 182.3 mAh/g at the C/10 rate for x = 0.2 Cu substitution. The

cycling measurements at 50C exhibit worse capacity fade when compared to

the measurements performed under ambient conditions. The in situ infrared

thermal imaging measurements for the cell that had the highest performance

in this study were performed for a constant voltage of 4.3 V for charging and

1.5 V for discharging of the cell. The ohmic heat was calculated from chronoamperometry

measurements, and the heat generation was fitted with the quadratic

term in the system.