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Chapter 11
is observed with a change in the cryolite ratio. An increase in the cryolite
ratio, causes a decrease in the cathodic overvoltage. These findings are
related to the laboratory experiments.
In industrial cells, the diffusion overvoltage is significantly lower, due to
convection. Thonstad estimated the cathodic overvoltage at about 100 mV.
Due to enrichment of the cathodic diffusion layer with sodium fluoride, it is
expected that electrowon aluminum metal contain higher concentration of
sodium than the amount corresponding to that of the equilibrium data for the
electrolyte (bulk melt). Most researchers have estimated that an average of
sodium is about 80 ppm, which is below the equilibrium data.
At current densities, which are normally used in the production of
aluminum, the primary gas evolved at the anode is At lower current
densities formation of CO in high contents may occur.
Anodic processes in the production of aluminum metal have received far
more attention than the cathodic processes. This comes as a consequence of
the complexity of anodic processes. However, despite the relatively active
research that has gone on the study of these processes, there is no general
agreement among published results nor between explanations of the behavior
observed, which is often associated with poor reproducibility.
For the purpose of studying the anodic reactions involved in alumina-
cryolite melts, the following electroanalytical procedures have been
investigated: chronoamperometry, chronopotentiometry, cyclic voltammetry,
impedance spectroscopy and related electrochemical methods.
8
Materials
used for the study of anodic reactions include various types of carbon,
platinum, gold and refractory metals.
The anodic overvoltage on various types of carbon electrodes in cryolite-
alumina melts was studied by steady-state measurements. Tafel slopes and
exchange current densities evaluated from these experiments depend on the
nature of the carbon materials. The reported overvoltages are very high. At
overvoltage values are 1.4 V, 1.0 V and 0.8 V for glassy carbon,
graphite and baked carbon, respectively.
7
The overvoltage increases with
decreasing porosity, which is attributed to a decrease in the wetted area.
The anodic overvoltage is higher on large anodes due to the shielding
effect of gas bubbles. Dewing and van der Kouwe
9
, as shown in Figure 11.1
for the graphite ATJ, found Tafel plots with slopes of 0.29.
As this figure shows, the exchange current varies from for
current densities below to for current densities above
The break between and is attributed to
changing ratio in the gas generated. At lower current densities, low
exchange current is due to adsorption of CO on the electrode surface. The
CO, which is produced by reaction of with dissolved aluminum, acts as
a catalytic poison. The fraction of CO in the gas will depend on how fast
is being generated electrochemically. At higher current densities, more
is produced, which leads to a dilution of CO and to a higher exchange