However, significant problems also attend the use of carbon anodes, related to their preparation and to their consumption during aluminum
smelting.
Arranging these materials for treatment exposes workers to injurious
carbon dust.
Consequently,
anode fabricators must undertake expensive filtering, collecting and treatment operations.
Moreover, interactions between the anode and the molten
electrolyte during
cell operation consume the anode.
Anode consumption is problematic for several reasons.
First, it makes
cell operation more difficult.
It is difficult to maintain uniform anode current loading during operation due to the continuously changing topology of the
electrolyte-anode interface.
Despite substantial effort, no fully satisfactory
inert anode has been identified.
While an
inert anode has been viewed as a highly desirable target, its discovery would provide an enhancement to an already-workable
system—not a pre-requisite for a viable process.
Although the FFC process moves in the right direction by obviating chlorination of
titanium dioxide it is nonetheless environmentally suspect due to the
halide electrolyte.
Also, the FFC process has not become economically viable owing to the long times required to remove all the
oxygen from the cathode,
solid-state
diffusion being extremely slow.
However, such high temperatures and highly corrosive conditions constitute a set of design constraints even more stringent than those for an
inert anode for the comparatively benign physicochemical climate of the Hall-Héroult cell.
Even if the standard noble metals—gold, silver and
platinum—were not conventionally regarded as prohibitively expensive for large-scale industrial applications, they would not be suitable candidates for use in a liquid titanium cell owing to either their relatively low melting temperatures (silver and gold) as compared with that of titanium or, in the case of
platinum, to its lack of
structural integrity.
Beyond designating an inert anode, the design of apparatus for electrolytic extraction from oxide media poses many challenges not faced in the Hall-Héroult cell.
Considering titanium again as an illustrative example, materials that may be serviceable at aluminum's relatively low
melting temperature may well lack
structural integrity at the higher temperatures—exceeding 1700° C.—required for deposition of
titanium metal in liquid form.
The
carbon substrate of the Hall-Héroult cell is not compatible with reactive metals such as titanium in this instance because these metals react, to an undesirable extent, with carbon to form carbides.
If the electronic conductance of this element is too low,
metal deposition at a commercially acceptable rate will be achieved only by application of a large
voltage, which in turn will translate into unacceptably high
electric power cost.
However, RHMs have other properties that detract from their suitability for cathode support in electrolytic cells: RHMs are expensive and also mechanically brittle and therefore difficult to shape.
To date, no material has been shown to meet the performance and practical requirements for a cathode substrate in a cell containing an oxide melt at temperatures exceeding 1700° C.