An investigation of the electrochemical intercalation of lithium into a Li1-delta CoO2 electrode based upon numerical analysis of potentiostatic current transients
Hc. Shin et Si. Pyun, An investigation of the electrochemical intercalation of lithium into a Li1-delta CoO2 electrode based upon numerical analysis of potentiostatic current transients, ELECTR ACT, 44(13), 1999, pp. 2235-2244
Lithium insertion into a porous Li1-deltaCoO2 electrode was investigated by
numerical analysis of potentiostatic cathodic current transients. As lithi
um was intercalated, the current transients at first exhibited two-stage be
havior in the presence of a single phase. This was later replaced by a thre
e-stage character when a Li-diluted alpha phase coexisted with a Li-concent
rated beta phase. From the comparison of derivatives of the experimental lo
garithmic current transients with those numerically simulated, it is sugges
ted that the chemical diffusivity of lithium ion predominantly determines t
he shapes of the first stage of the current transients when the two phases
coexist and of the later stage of the current transients when only a single
phase exists. The derivatives of the second stages of the linear and logar
ithmic current transients during the coexistence of two phases were observe
d to be characterized by an upward concave shape, indicating that lithium i
nsertion proceeds via phase boundary movement (PBM). Transition times t(tr(
1)) and t(tr(2)) were determined as the times of the local maxima on the de
rivatives of the experimental linear and logarithmic transients, respective
ly. These time values correspond to the onset and end of the PBM. The curre
nt transient and its derivative were simulated as functions of equilibrium
stoichiometry through the numerical analysis for lithium transport under th
e condition for potentiostatic lithium injection into the electrode subject
ed to the limitation placed by the 'pinning' of the phase boundary and the
impermeable constraint to lithium. The numerically simulated current transi
ent and the derivative of the second stage of the transient qualitatively m
atched those experimentally determined as functions of applied potential in
their three-stage character and upward concave shape, respectively. (C) 19
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