Journal of Power Sources 188 (2009) 296–300
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Journal of Power Sources
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Short communication
Influence of the cooling rate on the ageing of lead–calcium alloys
F. Rossi
a,∗
, M. Lambertin
a
, L. Delfaut-Durut
b
, A. Maitre
c
, M. Vilasi
d
a
LaBoMaP, Arts et Métiers ParisTech, Rue porte de Paris, 71250 Cluny, France
b
CEA, centre de Valduc [SEMP, LECM], 21120 Is-sur-Tille, France
c
SPCTS, UFR Sciences et Techniques, 87060 Limoges, France
d
LCSM, Université Nancy I, 54506 Vandoeuvre les Nancy, France
article info
Article history:
Received 11 September 2008
Received in revised form 3 November 2008
Accepted 15 November 2008
Available online 21 November 2008
Keywords:
Lead–calcium
Process parameters
Cooling rate
Ageing
Resistivity
Hardness
abstract
Cast lead–calcium alloys were known to be sensitive to experimental parameters, which cause large
variations on the ageing and overageing behaviour. From the study of these parameters, the quenching
rate was the only significant parameter. A critical cooling rate was defined based on hardness, electrical
resistivity and metallographical observations. The inconsistencies in the literature noticed on the evo-
lutions of lead–calcium alloys can now be explained by whether or not this critical cooling rate was
respected.
© 2008 Elsevier B.V. All rights reserved.
1. Introduction
Calcium has been used to significantly improve the mechanical
properties of lead by precipitation hardening from an oversaturated
solid solution. Numerous studies have been done on the subject
since the replacement of lead–antimony alloys by lead–calcium
alloys in the lead-acid batteries [1–4]. Research has dealt with
the determination of the mechanisms and the kinetics of harden-
ing and softening transformations. The behaviour of the alloy is
now well-explained [5] with the identification of five transforma-
tions.
The hardening was performed in three stages with (Fig. 1):
•
A: a first discontinuous transformation initiated on the grain
boundaries and sweeping the grains. The hardness of the alloy
increases from 6 HV (Hardness Vickers) to 10 HV,
•
B: a second incomplete and approximately 10 times slower trans-
formation named “puzzling” lets the hardness increase by 2 HV,
•
C: a last hardening process with the microprecipitation of Pb
3
Ca
(structure L1
2
) with mean size of 2.5 nm. The maximum hardness
is about 15 HV.
∗
Corresponding author. Tel.: +33 3 85 59 53 13; fax: +33 3 85 59 53 70.
E-mail address: rossi@cluny.ensam.fr (F. Rossi).
The hardening was then followed by two softening transforma-
tions (overageing) with (Fig. 1):
•
D: a coarsening of macroprecipitates aligned in strings. Their
growth is due to the progressive dissolution of the thin hardening
precipitates (state C),
•
E: a final softening with the coarsening of the macroprecipitates
to form lamellar (Pb
3
Ca) structures.
Among the studies on these alloys, many inconsistencies
remained during decades on the identification of the transforma-
tions. Differences in the observations and interpretations arise on
the one hand from the numerous transformations undergone by
these alloys and the inherent difficulties in working on lead alloys
(soft material and transformations kinetics in a range of several
minutes to several years at room temperature). On the other hand,
differences in behaviour have been attributed to the sensitivity of
the alloy to its chemical composition and its thermal history. We
have studied the effect of the process and heat treatment parame-
ters on the transformation of the alloy. Experiments were designed
to study the effect of each parameter (casting temperature of the
alloy, preheating temperature of the mould, temperature of the
quenching bath, etc.) [5]. Results have shown that most of the pro-
cess parameters had no significant effect on the transformations of
the alloy except the quenching rate. This paper is devoted to the
analyses of the effect of this main parameter.
0378-7753/$ – see front matter © 2008 Elsevier B.V. All rights reserved.
doi:10.1016/j.jpowsour.2008.11.049