TY - JOUR
T1 - Investigation of the high-frequency resistance of a lead-acid battery
AU - Huet, F.
AU - Nogueira, R. P.
AU - Lailler, P.
AU - Torcheux, L.
N1 - Funding Information:
The authors would like to acknowledge the financial support of CEAC and ADEME (Convention No. 99-05-081).
PY - 2006/8/25
Y1 - 2006/8/25
N2 - The high-frequency resistance, RHF, or internal resistance, of 45 Ah flooded tubular lead-acid battery (LAB) cells was monitored during cycling at constant rates between C/100 and C/10 in order to understand the origin of the RHF variations and to evaluate the feasibility of monitoring the state-of-charge (SOC) with this parameter. It is shown that the RHF variations did not depend on the electrolyte-conductivity variations, as usually indicated in the literature. At a low discharging rate (C/100), RHF increased only at low SOCs, with a high final value, while at a high rate (C/10) RHF increased progressively from the beginning of the discharge, with a low final value. This has been interpreted as the consequence of the shape and size of the PbSO4 crystals in the pores of the active material, which are the result of the continuous competition between crystal nucleation and crystal growth. RHF informs on the structure of the PbSO4 layer, and therefore, depends strongly on the history of the previous cyclings of the cell. Monitoring the SOC from the single value of RHF was found to be impossible since, for different cycling rates, distinct values of SOC may correspond to the same value of RHF. Fluctuations of RHF were also measured at different SOC: they allow detection of gas evolution in the cell and could provide complementary information for estimating the SOC of LABs.
AB - The high-frequency resistance, RHF, or internal resistance, of 45 Ah flooded tubular lead-acid battery (LAB) cells was monitored during cycling at constant rates between C/100 and C/10 in order to understand the origin of the RHF variations and to evaluate the feasibility of monitoring the state-of-charge (SOC) with this parameter. It is shown that the RHF variations did not depend on the electrolyte-conductivity variations, as usually indicated in the literature. At a low discharging rate (C/100), RHF increased only at low SOCs, with a high final value, while at a high rate (C/10) RHF increased progressively from the beginning of the discharge, with a low final value. This has been interpreted as the consequence of the shape and size of the PbSO4 crystals in the pores of the active material, which are the result of the continuous competition between crystal nucleation and crystal growth. RHF informs on the structure of the PbSO4 layer, and therefore, depends strongly on the history of the previous cyclings of the cell. Monitoring the SOC from the single value of RHF was found to be impossible since, for different cycling rates, distinct values of SOC may correspond to the same value of RHF. Fluctuations of RHF were also measured at different SOC: they allow detection of gas evolution in the cell and could provide complementary information for estimating the SOC of LABs.
KW - Electrochemical impedance
KW - Electrochemical noise
KW - High-frequency resistance
KW - Internal resistance
KW - Lead-acid battery
KW - State-of-charge
UR - http://www.scopus.com/inward/record.url?scp=33748114500&partnerID=8YFLogxK
U2 - 10.1016/j.jpowsour.2005.11.026
DO - 10.1016/j.jpowsour.2005.11.026
M3 - Article
AN - SCOPUS:33748114500
SN - 0378-7753
VL - 158
SP - 1012
EP - 1018
JO - Journal of Power Sources
JF - Journal of Power Sources
IS - 2 SPEC. ISS.
ER -