RECOVERY OF HEAVY METALS
FROM SPENT NICKEL-CADMIUM BATTERIES
Lia I.C. Barros, Adriano M.G. Pacheco*, and Fernanda Margarido
CVRM
- Mineral Resources Valorization Centre, Instituto Superior
Técnico
Av. Rovisco Pais 1, 1049-001 Lisboa, Portugal (* mail to: apacheco@ist.utl.pt)
Abstract
Ni-Cd cells remain the main sink for Cd production and, at the same
time, the major source of Cd pollution to the environment, which calls for an
improvement in its recovery. In this study, dismantled batteries underwent
granulometric separation by wet sieving, using an intense flow. Regardless of
the shredder’s output, results point to a major separation around 2.8-mm mesh.
Upper fractions still contain heavy metals though, therefore an additional
process is required. The infra fractions can proceed directly to the recovery
stages downstream. The amount of material in the finest fractions is inversely
proportional to the mesh of the shredder's output, yet this parameter appears
to have no influence on the granulometry of such fractions. Toxic metals (Cd,
Co, Ni) concentrate in the infra fractions, whereas ferrous and organic scrap
are retained above.
There is not much doubt about the significant increase
in collection rates of spent batteries in the European Union, following the EC
Battery Directive 91/157 EEC (1991). The present situation is still far from
being satisfactory though. In 1997, total EU take-back was up to 20,000 tons,
yet almost 30,000 tons (about 900 million portable units) were being sold every
year in the German market alone [2,3]. Related figures from other Member States
point to a collection rate of about 50-60 % at best, an efficiency that seems
unlikely to rise without some sort of economical incentive to end-users for
proper battery disposal [1,4]. Rate notwithstanding, an important amount of
toxic waste from spent cells will keep on getting into incinerators, landfills
and other general-purpose, disposal sites in the (near) future. Now the problem
for an average, small-to-medium country in a developed stage is that there are
only two alternatives: the former one, which means no chemical spillage – just
in the strict sense, of course…! – but also no metal recovery whatsoever, or
else feeding the spent cells into an undifferentiated, scrap battery (or scrap
metal) processing plant, which could mean some recovery yet involve some costly
and probably off-border operation, given the scarcity of specialised
reclamation facilities around the world.
The above considerations triggered the concept behind a current project
on metal recovery from spent Ni-Cd batteries, which this paper is about. That
and also an idea of putting together an all-inclusive operation, from scrap
batteries to value metals, which could avoid high temperature processing and
huge plants, and rather fit into small-to-medium scale units without loss of
profitability. The Project runs on a multi-partnership basis, involving people
and resources from a technical university, a national laboratory and a private
corporation, with financial support from the Portuguese Government and the
European Union. Major research tasks are:
i. Physical
processing of spent batteries, in order to optimize the granulometry and the
recyclable content downstream.
ii. Hydro-electrometallurgical
processing of battery scrap into nickel, cadmium and cobalt forms, as pure as
possible.
iii. Assembly
of unit operations into a laboratory-scale prototype for the whole
metal-recovery process.
iv. Technical
and economic audits.
The present paper will focus on the physical-processing stage. The separation
techniques as well as the characterization of the resulting fractions are
presented and discussed, especially in what matters to the easing of subsequent
operations.
The study herein deals
with the initial (physical) stage of an integrated process for recovering Cd,
Ni and Co from spent Ni-Cd batteries. All experiments refer to small batteries
of the cylindrical, sealed type, picked up at random from batches of
fully-exhausted devices that had been used in campaign radios by the Portuguese
Army. Each unit weighs 150±5 g and has a bright-yellow, plastic
cover. Cells were dismantled by means of a single-shaft disintegrator (ERDWICHâ; model: EWZ 200), with interchangeable output sieves of 20,
10 or 6 mm. The resulting material underwent granulometric separation by wet
sieving (down to 0.355 mm), using an intense water flow
(10 l min-1) and FRITSCHâ sieves (DIN 4188 series) of 1.4, 2.0, 2.8, 4.0, 5.6 e
8.0 mm.
The samples mass
was determined through the Pierre Gy
Theory [8].The
granulometry of the fractions under 0.355 mm, resulting from wet sieving with
moderate flow experiments, were checked out by laser diffraction analysis,
using a CILASä 920 analyzer. Samples dismantled with
the three output sieves were analyzed. Optical and scanning
electron microscopy with an energy-dispersive probe (SEM/EDS) were used for
morphological and chemical characterization of all fractions.
This
operation promotes a first splitting between the value metallic material (Cd,
Ni and Co) and the scrap (metallic case, plastic wrap and the electrode
material supporting grates). Two fractions are obtained – the upper and the
infra. There are no significant differences between them,
only the upper one usually comes richer in plastic cover and metallic case. In
an industrial process, however, some advantage could be taken of handling the
two fractions separately. The volume of dismantled material decreases
proportionally to the mesh of the shredder's output sieve. The hardness of the
material, as well as the cutting process itself, leads to a random distribution
of components in either fraction, which makes it difficult to work out an
association (if any…) between material losses and such an output.
Results from wet sieving and laser granulometry (<
0.355 mm) are summarized in Figures 1 and 2,
respectively.


Fig.
2 - Simple histograms of the infra and upper fraction
distribution as a function of the used separation sieve.
Up to 2.8 mm sieve
included, the upper fraction amount is always bigger than the infra one,
whatever output shredder’s sieve is used. From the 5.6 mm up to 10 mm sieve,
this situation is inverted only for the material dismantled with the smaller
mesh shredder’s output sieve (6 mm). In all wet-sieving experiments, the mass
difference between upper and infra fraction diminishes with the dimension of
the shredder’s output sieve mesh. In the assays using the 1.4 , 2 and 2.8 mm
sieves, a very little amount of plastic and practically no metallic case
appears in the infra fraction. Infra 4 mm fraction already contains some grate
but, still thus, its composition does not differ significantly from the
previous fraction (infra 2.8 mm). Anyway, the plastic is not problematic,
therefore its splitting is relatively simple, since is the only not magnetic
component of the batteries. For 5.6 , 8 and, mainly, 10 mm sieves, the amount
of grate and metallic case in the infra fraction is very high and the splitting
between the components moves away, each time more, from the desired one. This
situation occurs, probably, because these values are similar to the shredder’s
output sieves dimensions, despite the difference in mesh geometry. Thus, based
in the obtained results, it can be concluded that, for wet-sieving operation
using the assayed water flow, the cut-off value rounds 2.8 mm or, at the most,
4 mm.


Fig. 2 – Cumulative plots of
grain size and population density distribution for the wet sieving finer fraction.
On the basis of the
obtained results it may be concluded that shredder’s output sieve dimension
does not influence the finest material fractions granulometry, but only its
amount, which is inversely proportional to the sieve’s mesh dimension. Being
the main objective to obtain the biggest amount of individualized metallic dust
of the remainder material, the use of 6 mm shredder’s is far more adjusted.
However, in this case, the plastic and the metallic case appear, especially in
the upper fraction, in smal ler particles, witch can turn its recovery far more
difficult.
After analyzing the different batteries components, we find plastics and metallic crap; value metals reduced to dust and their respective supporting grate constitute the electrodes. A different coloration between the anode (clear grey) and the cathode (dark grey) is visible. Both materials present a strong tack to the supporting grate, specially the anodic one, making more difficult its full splitting. Figure 3 presents microphotographs obtained in the Scanning Electron Microscope, evidencing the most common morphologies of the anodic and cathodic material. These samples were subjected to mechanical dismantling, followed by wet-sieving with moderate water flow [6]. The X-ray spectrum obtained by Energy Dispersive Spectrometry (EDS), for details of anodic and cathodic material, are showed in Figure 4.


a)
b)
Fig. 3 – Scanning Electron
Microscope microphotograph of the electrode material:
a)
anodic
(2000x); b) cathodic (1000x).


a) b)
Fig. 4 – Electrode material X-ray
spectra, obtained by Energy
Dispersive Spectrometry:
a) anodic; b) cathodic.
The
anodic and cathodic material appears in the samples with varied morphologies,
but it is not very difficult to distinguish them: the anodic material evidences
a more compact and geometric structure that the cathodic one. Then it is
comprehensive that this offers the biggest resistance to the splitting from the
respective supporting grate. The spectra analysis enables to verify that the
anodic material grains are essentially constituted by cadmium. The supporting
grate is constituted by iron and nickel. The cathodic material is essentially
composed by nickel, some cadmium and a small amount of cobalt.
Conclusions
All experiments herein refer to single-sieve wet sieving tests, using an
intense water flow - 10 Lmin-1 - during 2 minutes. Another
experiments already described [6] were done with different experimental
conditions: using a sieve serie and a 1Lmin-1 washing water flow for
over 30 minutes In the first experiments the separation between scrap (iron and organic
material) and the value metals (Cd, Co, Ni) occurred, mainly, at the 1.4 mm
sieve level, despite of the shredder’s output sieve mesh dimension. The use of
an intense water flow made possible to increase the cut-off value for 2.8 mm,
or even 4 mm, which constitutes, from the technical-economic point of view, a
more viable solution. According to this experiments, it can be verified that
the intense water flow wet sieving operation is the most adjusted after the
dismantling, allowing to clean the scrap (plastic and metallic case) from the
metallic dust. Therefore, a magnetic process (for example) can easily do these
components removal. It was not possible to achieve full splitting of the electrode
material from the respective supporting grate, even when an intense water flow
was used. Thus, it will be necessary to apply for chemical processes. Leaching
assays will be able to constitute an important contribution to the splitting
process. Regarding to the organic fiber, is separation from electrode metals
seems fundamental, since it can turn impracticable their reuse. In this phase,
the definitive choice of the optimal shredder’s output sieve mesh, as well as a
definitive wet-sieving cut-off value, can not be put to stray. The final
conclusions can only be made when subsequent stages of grain size analysis and,
over all, chemical (leaching and solvent extraction) and electrochemical
splitting experiments come to an end.
Acknowledgements
The work, which this
paper refers to, has been financially supported by the Foundation for Science
and Technology (FCT; Portugal) under the contract PRAXIS XXI 3/3.1/CEG/2574/95.
Lia Barros acknowledges a research scholarship (PRAXIS
XXI/BIC/17099/98) from FCT as well. The Authors are indebted to the Portuguese
Army (DGMT) for providing the raw material (spent batteries) for this
continuing study.
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