A theory of the grid/positive active-mass (PAM) interface and possible methods to improve PAM utilization and cycle life of lead/acid batteries

Abstract Very often, the cycle life of batteries with antimony-free positive grids operating under deep-discharge cycling is determined by the grid/PAM interface. The properties of this interface are overviewed and the technological and design parameters influencing these properties, and hence determining the cycle life of the battery, are discussed. A new parameter γ is proposed. This is defined as grams of PAM per 1 cm2 of grid-collector surface area. It has been established that the grid/PAM interface consists of two layers, namely, a corrosion layer (CL) and a layer of the active mass that collects the current from the remaining (capacity-bearing) part of the PAM (AMCL). The technological parameters that influence the specific resistivity of both CL and AMCL, as well as the surface area of the layers through which current flows between the PAM and the collector are discussed. On the basis of the principles derived from the theory of the grid/PAM interface, batteries are produced and tested.

[1]  D. Pavlov,et al.  The PbO2 Particle: Exchange Reactions Between Ions of the Electrolyte and the PbO2 Particles of the Lead‐Acid Battery Positive Active Mass , 1992 .

[2]  J. S. Anderson,et al.  The intermediate oxides of lead , 1959 .

[3]  Robert F. Nelson,et al.  Pure lead and the tin effect in deep-cycling lead/acid battery applications , 1991 .

[4]  D. Pavlov,et al.  Influence of Antimony on the Structure and the Degree of Hydration of the Anodic PbO2 Layer Formed on Pb‐Sb Electrodes , 1994 .

[5]  D. Pavlov,et al.  Dependence of the phase composition of the anodic layer on oxygen evolution and anodic corrosion of lead electrode in lead dioxide potential region , 1978 .

[6]  D. Pavlov,et al.  Hydrated structures in the anodic layer formed on lead electrodes in H2SO4 solution , 1993 .

[7]  D. Pavlov,et al.  The Lead‐Acid Battery Lead Dioxide Active Mass: A Gel‐Crystal System with Proton and Electron Conductivity , 1992 .

[8]  T. Rogachev Effect of antimony on the anodic corrosion of lead and oxygen evolution at the Pb/PbO2/H2O/O2/H2SO4 electrode system , 1988 .

[9]  Detchko Pavlov,et al.  Suppression of premature capacity loss by methods based on the gel—crystal concept of the PbO2 electrode , 1993 .

[10]  A. Hollenkamp,et al.  Effects of grid alloy on the properties of positive-plate corrosion layers in lead/acid batteries. Implications for premature capacity loss under repetitive deep-discharge cycling service , 1994 .

[11]  K. Bullock,et al.  Corrosion of Lead in Sulfuric Acid at High Potentials , 1986 .

[12]  F. Lappé Some physical properties of sputtered PbO2 films , 1962 .

[13]  D. Pavlov,et al.  Mechanism of the action of Ag and As on the anodic corrosion of lead and oxygen evolution at the Pb/PbO(2−x)/H2O/O2/H2SO4 electrode system , 1986 .

[14]  D. Pavlov,et al.  The effect of antimony on the anodic behaviour of lead in H2SO4 solution , 1991 .

[15]  Mario Maja,et al.  Mechanism of Action of Sn on the Passivation Phenomena in the Lead‐Acid Battery Positive Plate (Sn‐Free Effect) , 1989 .

[16]  D. Pavlov,et al.  Hydration and Amorphization of Active Mass PbO2 Particles and Their Influence on the Electrical Properties of the Lead‐Acid Battery Positive Plate , 1989 .

[17]  D. Pavlov Effect of corrosion layer on phenomena that cause premature capacity loss in lead/acid batteries , 1994 .

[18]  B. K. Mahato,et al.  The Cyclic Corrosion of the Lead‐Acid Battery Positive , 1979 .

[19]  D. Pavlov,et al.  A Model of the Structure of the Positive Lead‐Acid Battery Active Mass , 1984 .

[20]  W. Mindt,et al.  Electrical Properties of Electrodeposited PbO2 Films , 1969 .

[21]  Masaharu Tsubota,et al.  Physical Changes in Positive Active Mass during Deep Discharge‐Charge Cycles of Lead‐Acid Cell , 1983 .

[22]  David A. J. Rand,et al.  Discussions on the lead/acid battery system , 1988 .