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Accumulateur Lithium Soufre

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Accumulateur Lithium Soufre ( accumulateur-lithium-soufre )

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Chapter 6: EIS and low temperature studies Figure 6-3. Nyquist plots of Li/S cell: comparison of experimentally measured data (in black) with the calculated one (in red). Firstly, the S8||S8 response is mainly dominated by a blocking behavior, which gives the low frequency contribution in the complete Li/S cell. It exhibits a very small semicircle (~ 2 Ω) at quite high frequencies, i.e. at the characteristic frequency of ~ 9 kHz, instead of 600 Hz in the complete cell. This loop was previously interpreted (chapters 2 and 3) as characteristics of the electron transport in the electronic pathway in the positive electrode. In any cases, the contribution of the positive electrode resistance to the MF loop of complete Li/S cell is very small, and cannot be distinguished in the overall response. On the contrary, we can note that the characteristic frequency of the semicircle in a complete cell (Li/S) and symmetric Li||Li cell are almost identical, and their amplitudes are very similar (in the range of ~ 100 Ω). Therefore, the loop in the MF range (of Li/S cell) can be attributed to the lithium negative electrode, with a main contribution coming from the passivation layer on the lithium surface225,248. Once could also notice the presence of a semicircle in the LF region for the symmetric Li||Li cell (Figure 6-2b, red curve). The literature often attributes this LF semicircle to the charge transfer occurring on the negative electrode225,248. In our case however, we cannot really correlate it with the charge transfer and corresponding double layer capacitance. We roughly estimated the capacitance of this semicircle according to equation (23): < ∙ T ∙ U = 1 (21) < ∙ V ∙ UW = 1 (22) (23) If considering α ~ 0.575 and R ~ 160 Ω (obtained from LF semicircle fitting), a capacitance value of ~ 1·10-3 F cm-2 was found. Assuming that for a charge transfer resistance process, a 195 Resistor in parallel with pure Capacitor (C) relation: Resistor in parallel with a Constant Phase Element (CPE) relation: T=<(WMLM) ∙VWM

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