TY - JOUR
T1 - Chronoamperometric measurements and modeling of nucleation and growth, and moving boundary stages during electrochemical lithiation of graphite electrode
AU - Levi, M. D.
AU - Markevich, E.
AU - Wang, C.
AU - Aurbach, D.
PY - 2007/2/1
Y1 - 2007/2/1
N2 - Chronoamperometric studies of the stage 2 (LiC12) to stage 1 (LiC6) transition during electrochemical insertion of Li ions into graphite electrodes showed 5 distinct domains in their current vs. time curves. A linear increase of current at the beginning of domain II and a decrease in current with time within domain IY were identified with two-dimensional instantaneous nucleation of cylindrical grains of stage 1 into stage 2, their growth and further coalescence with the formation of the continuous moving boundary. We could calculate the following characteristic parameters: the nucleation time constant, τn = 990 s; the density of nucleation sites No = 2.5 × 108 cm-2, the velocity of the lateral growth of cylindrical nuclei, a = 3.6 × 10-8 cm s-1 and the thickness of the nucleation layer, d = 0.36 μm. After nucleation stage, the interphase propagates initially linearly with time and then proportionally to the square root of time (domain IV). At 30 °C the speed of propagation of the moving boundary between stage 1 and stage 2, dξ/dt′, is around 1.6 × 10-7 cm s-1. The activation energies of a, dξ/dt′ and D1 obtained from the related Arrhenius plots were found to be 0.13, 0.19 and 0.23 eV, respectively.
AB - Chronoamperometric studies of the stage 2 (LiC12) to stage 1 (LiC6) transition during electrochemical insertion of Li ions into graphite electrodes showed 5 distinct domains in their current vs. time curves. A linear increase of current at the beginning of domain II and a decrease in current with time within domain IY were identified with two-dimensional instantaneous nucleation of cylindrical grains of stage 1 into stage 2, their growth and further coalescence with the formation of the continuous moving boundary. We could calculate the following characteristic parameters: the nucleation time constant, τn = 990 s; the density of nucleation sites No = 2.5 × 108 cm-2, the velocity of the lateral growth of cylindrical nuclei, a = 3.6 × 10-8 cm s-1 and the thickness of the nucleation layer, d = 0.36 μm. After nucleation stage, the interphase propagates initially linearly with time and then proportionally to the square root of time (domain IV). At 30 °C the speed of propagation of the moving boundary between stage 1 and stage 2, dξ/dt′, is around 1.6 × 10-7 cm s-1. The activation energies of a, dξ/dt′ and D1 obtained from the related Arrhenius plots were found to be 0.13, 0.19 and 0.23 eV, respectively.
KW - Current transients
KW - Electrocrystallization
KW - Nucleation rate
KW - Two-phase coexistence
UR - http://www.scopus.com/inward/record.url?scp=33846228456&partnerID=8YFLogxK
U2 - 10.1016/j.jelechem.2005.11.037
DO - 10.1016/j.jelechem.2005.11.037
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AN - SCOPUS:33846228456
SN - 1572-6657
VL - 600
SP - 13
EP - 22
JO - Journal of Electroanalytical Chemistry
JF - Journal of Electroanalytical Chemistry
IS - 1
ER -