BACKGROUND OF THE INVENTION
1 - Field Of The Invention
[0001] The invention relates to improved non-consumable electrodes, particularly for use
in the production of aluminum in Hall-Heroult cells, and to a method for achieving
a uniform current density on the electrode working surface. 2 - Description Of The
Prior Art
[0002] Aluminum is conventionally produced in Hall
-Heroult cells by the electrolysis of alumina in molten cryolite, using conductive
carbon electrodes. During the reaction, the carbon anode is consumed at the rate of
approximately 450 kg/mT of aluminum produced under the overall reaction
[0003]

[0004] The problems caused by the use of carbon anodes are related to the cost of the anode
consumed in the above reaction and to the impurities introduced to the melt from the
carbon source. The petroleum cokes used in the fabrication of the anodes generally
have significant quantities of impurities, principally sulfur, silicon, vanadium,
titanium, iron and nickel. Sulfur is oxidized to its oxides, causing troublesome workplace
and environmental pollution problems. The metals, particularly vanadium, are undesirable
as contaminants in the aluminum metal produced. Removal of excess quantities of the
impurities requires extra and costly steps when high purity aluminum is to be produced.
[0005] If no carbon were consumed in the reduction the overall reaction would be 2Al
2O
3 → 4Al + 30
2 and the oxygen produced could theoretically be recovered. More importantly, with
no carbon consumed at the anode there would be no contamination of the atmosphere
or the product from the impurities present in the coke.
[0006] Attempts have been made in the past to use non-consumable electrodes with little
apparent success. Metals either melt at the temperature of operation, or are attacked
by oxygen and/or the cryolite bath. Ceramic compounds, such as oxides with perovskite
and spinel crystal structures, usually have too high electrical resistance or are
attacked by the cryolite bath.
[0007] Previous efforts in the field are disclosed in U.S. 3,718,550-Klein, Feb. 27, 1973,
Cl. 204/67; U.S. 4,039,401-Yamada et al., Aug. 2, 1977, Cl. 204/67; U.S. 2,467,144-Mochel,
April 12, 1949, Cl. 106/55; U.S. 2,490,825-Mochel, Feb. 1, 1946, Cl. 106/55; U.S.
4,098,669-de Nora et al., July 4, 1978, Cl. 204/252; Belyaev + Studentsov, Legkie
Metal 6, No. 3, 17-24 (1937), (C.A. 31 [1937], 8384) and Belyaev, Legkie Metal 7,
No. 1, 7-20 (19381 (C.A. 32 [1938], 6553).
[0008] Of the above references, Klein discloses an anode of at least 80% SnO
2, with additions of Fe203, ZnO, Cr
203, Sb203,
Bi203, V
2O
5, Ta
2O
5, Nb
20
5 or W0
3. Yamada discloses spinel structure oxides of the general formula XYY'O
4 and perovskite structure oxides of the general formula RMO
3, including the compounds CoCr
20
4, TiFe
2O
4, NiCr204, NiCo
2O
4, LaCrO
3, and LaNiO
3. Mochel discloses SnO
2 plus oxides of Ni, Co, Fe, Mn, Cu, Ag, Au, Zn, As, Sb, Ta, Bi and U. Belyaev discloses
anodes of Fe203, SnO
2, Co
30
4, NiO, ZnO, CuO, Cr
2O
3 and mixtures thereof as ferrites. De Nora dis
- closes Y
20
3 with Y, Zr, Sn, Cr, Mo, Ta, W, Co, Ni, Pd, Ag, and oxides of Mn, Rh, Ir, and Ru.
[0009] The Mochel patents relate to electrodes for melting glass, while the remainder are
intended for high temperature electrolysis, such as Hall-Heroult aluminum reduction.
Problems with the materials above are related to the cost of the raw materials, the
fragility of the electrodes, the difficulty of making a sufficiently large electrode
for commercial usage, and the low electrical conductivity of many of the materials
above when compared to carbon anodes.
[0010] U.S. 4,146,438, March 27, 1979, de Nora et al., Cl. 204/1.5, discloses electrodes
comprising a self-sustaining body or matrix of sintered powders of an oxycompound
of at least one metal selected from the group consisting of titanium, tantalum, zirconium,
vanadium, niobium, hafnium, aluminum, silicon, tin, chromium, molybdenum, tungsten,
lead, manganese, beryllium, iron, cobalt, nickel, platinum, palladium, osmium, iridium,
rhenium, technetium, rhodium, ruthenium, gold, silver, cadmium, copper, zinc, germanium,
arsenic, antimony, bismuth, boron, scandium and metals of the lanthanide and actinide
series and at least one electroconductive agent, the electrodes being provided over
at least a portion of their surface with at least one electro- catalyst.
[0011] U.S. Patent No. 3,930,967-Alder, January 6, 1976, Cl. 204/67, discloses bi-polar
electrodes made by sintering formed mixtures of Sn0
2, as a principal component, with small percentages of Sb
20
3, Fe
20
3 and CuO.
[0012] U.S. Patent No. 3,960,678-Alder, June 1, 1976, Cl. 204/67, discloses a Hall-Heroult
process using an anode having a working surface of ceramic oxide, wherein a current
density above a minimum value is maintained over the whole anode surface to prevent
corrosion. The anode is principally Sn0
2, preferably 80.0 to 99.7 wt. %. Additive oxides of Fe, Cu, Sb and other metals are
disclosed.
[0013] U.S. Patent No. 4,057,480-Alder, November 8, 1977, Cl. 204/290 R, a divisional application
from U.S. Patent No. 3,960,678, relates to a ceramic oxide anode for a Hall-Heroult
cell using a current density maintained above a minimum value over the contact surface
of the anode. A protective ring is fitted over the three phase zone at the air-electrolyte-
anode junction. Anode base material is Sn0
2, 80.0-99.7 wt. % is shown with additions of 0.05-2.0 wt. % of oxides of Fe, Cu, Sb
and other metals as dopants.
[0014] U.S. Patent No. 4,233,148-Ramsey et al., November 11, 1980, Cl. 204/291, discloses
electrodes suitable for use in Hall-Heroult cells composed of SnO
2 with various amounts of conductive agents and sintering promoters, principally Ge0
2, Ca
3O
4, Bi
2O
3, Sb
2O
3, MnO
2, CuO,
Pr203' In
2O
3 and MoO
3.
[0015] Despite the efforts described above, preparation of usable electrodes for Hall-Heroult
cells still has not been fully realized and no instance is known of any plant scale
commercial usage. The spinel and perovskite crystal structures have in general displayed
poor resistance to the molten cryolite bath, disintegrating in a relatively short
time. Electrodes consisting of metals coated with ceramics using conventional methods
have also shown poor performance, in that almost inevitably, even the smallest crack
leads to attack on the metal substrate by the cryolite, resulting in spalling of the
coating, and consequent destruction of the anode.
[0016] The most promising developments to date appear to be those using stannic oxide, which
has a rutile crystal structure, as the basic matrix. Various conductive and catalytic
compounds are added to raise the level of electrical conductivity and to promote the
desired reactions at the working surface of the anode.
[0017] A major cause of the difficulties experienced with the use of conductive anodes having
flat working surfaces in Hall-Heroult cells is the high current densities that exist
at the edges and corners of the anodes. As a result, the operating life of these anodes
is shortened by selective attack of these regions by the molten electrolyte bath.
Regarding anodes having a protective surface covering, it has been accepted and common
practice to utilize a material of very high electrical resistivity for the covering,
compared to the resistivity of the protected material.
[0018] The primary objective of the invention is to provide an improved electrode having
a substantially flat working surface and wherein a uniform current density exists
at all available regions of the working surface of the electrode during operation
thereof in a molten salt electrolysis cell. The uniform current density inhibits selective
attack of the electrode and provides improved process control.
[0019] It is another objective of the invention to provide an improved electrode wherein
the requirement of large differences between the electrical resistivity of the core
and core-protecting material is greatly relaxed.
[0020] Another objective of the invention is to provide an improved method for manufacturing
aluminum by the electrolysis of alumina in molten cryolite in a Hall-Heroult cell
employing a non-consumable anode comprising the electrode of the invention.
[0021] The invention in one aspect provides a non-consumable electrode particularly, but
not exclusively, suitable as an anode for a Hall-Heroult cell having a molten electrolyte
bath at cell operating temperature which essentially achieves a uniform current density
across its flat working surface, and may be produced from materials having a relatively
small difference in electrical resistivity. The electrode, and especially an anode
is generally produced by the process of: (a) forming, preferably by isostatic pressing,
a first conductive ceramic material to produce a core having a substantially flat
working surface and a non-working surface; (b) forming a physically adherent coating
over the non-working surface of the core on at least the portion thereof which is
to be exposed to the electrolyte bath in the cell, the coating consisting of a second
conductive ceramic material having a closely matching coefficient of thermal expansion,
a close matching of shrinkage during sintering, and a higher electrical resistivity
compared to the first conductive ceramic material and capable of being chemical diffusion
bonded thereto; and (c) sintering the coated core thus formed to produce a monolithic
ceramic electrode having a substantially flat working surface and a non-working surface,
the non-working surface having an impervious coating thereon, at least in the portion
thereof exposed to the electrolyte bath, of higher resistivity than the core and chemical
diffusion bonded thereto, whereby substantially all of the current applied to the
electrode is conducted into the electrolyte bath through the flat working surface.
[0022] The invention also provides a method for manufacturing aluminum by the electrolysis
of alumina in molten cryolite in a Hall-Heroult cell employing a non-consumable anode
which essentially achieves a uniform current density across its flat working surface,
and may be produced from materials having a relatively small difference in electrical
resistivity. The anode is generally produced by the process of: (a) forming, preferably
by isostatic pressing, a first conductive ceramic material to produce a core having
a substantially flat working surface and a non-working surface; (b) forming a physically
adherent coating over the non-working surface of the core on at least the portion
thereof which is to be exposed to the electrolyte bath in the cell, the coating consisting
of a second conductive ceramic material having a closely matching coefficient of thermal
expansion, a close matching of shrinkage during sintering, and a higher electrical
resistivity compared to the first conductive ceramic material and capable of being
chemical diffusion bonded thereto; and (c) sintering the coated core thus formed to
produce a monolithic ceramic anode having a substantially flat working surface and
a non-working surface, the non-working surface having an impervious coating thereon,
at least in the portion thereof exposed to the electrolyte bath, of higher resistivity
than the core and chemical diffusion bonded thereto, whereby substantially all of
the current applied to the anode is conducted into the electrolyte bath through the
flat working surface.
[0023] The phrase "physically adherent coating over the non-working surface of the core"
refers to a coated core possessing sufficient integrity such that it can be handled
and shaped without separation of the coating from the core. A particularly suitable
method for applying an adherent coating is the isostatic pressing method. The adherence
in this case is derived from the physical interpenetration of coating and core materials
at the adjoining interface. Other coating methods, such as flame spraying or dipping,
which permit subsequent chemical diffusion bonding of the coating during sintering
may also be used.
[0024] The phrase "closely matching coefficient of thermal expansion" refers to the requirement
that the CTE of the coating and core materials of the electrode should differ by no
more than about 1.0 x 10 /°C. to prevent destruction of the electrode during use.
In a preferred system, the . CTE difference is limited to no more than about 0.5%.
[0025] Likewise, the phrase "a close matching" of shrinkage refers to the requirement that
the coating and core materials must undergo an essentially equivalent dimensional
or volume change during sintering.
[0026] Chemical diffusion bonding as used herein is defined as the cohesion resulting from
the mutual migration of the coating and core constituents across an adjoining interface
to form an interphase region with chemical composition intermediate between that of
the coating and the core and compatible with each.
[0027] An electrode produced by our process which particularly lends itself to commercial
production involves:
(a) forming an elongated core having two ends from a first conductive ceramic material;
(b) forming a physically adherent coating over the core with a second conductive ceramic
material having a closely matching coefficient of thermal expansion, a close matching
of shrinkage during sintering, and a higher electrical resistivity compared to the
first conductive ceramic material and capable of being chemical diffusion bonded thereto;
(c) producing a substantially flat uncoated working surface on only one end of the
coated core by removing the coating therefrom; and
(d) sintering the coated core having a substantially flat uncoated working surface
to produce an integral monolithic body with an impervious coating layer, thereby forming
a ceramic electrode having a substantially flat working surface and a non-working
surface, the non-working surface having a coating of higher resistivity than the core
and chemical diffusion bonded thereto, whereby substantially all of the current applied
to the electrode is conducted into the electrolyte bath through the flat working surface.
The preferred method for forming the elongated core and physically adherent coating
is isostatic pressing.
[0028] The preferred conductive ceramic core composition for the electrode consists of 98.0-98.5
wt. % SnO
2, 0.1-0.5 wt. % CuO and 1.0-1.5 wt. % Sb
20
3. A particularly advantageous core composition consists of 98.5 wt. % Sn0
2, 0.5 wt. % CuO and 1.0 wt. % Sb203.
[0029] The preferred conductive ceramic coating material is an Fe
2O
3-doped Sn0
2 composition, preferably consisting of 98.00-99.75 wt. % SnO
2 and 0.25-2.00 wt. % Fe203, and ideally 98.0 wt. % SnO
2 and 2.0 wt. % Fe
203.
[0030] The following example will further describe the invention. It is understood that
this example is provided to illustrate the practice of the invention and is not intended
as limiting beyond the limitations imposed by the appended claims.
[0031] A powder mixture consisting of 985 grams Sn0
2, 5 grams CuO and 10 grams Sb
20
3 was wet milled for six hours, after which the resulting slurry was vacuum filtered
and dried by means well known in the art. The dried material was screened through
a sieve having openings of about 425 microns (40 mesh Tyler Screen Scale), and then
calcined at 900°C. in air to promote chemical reactivity and improve homogeneity.
The wet-milling, vacuum filtration, and drying steps were repeated to provide powdered
material with which to produce the anode core.
[0032] A powder mixture consisting of 980 grams Sn0
2 and 20 grams Fe
20
3 was treated in an identical manner as was used in the core material preparation described
above to produce a powder for use in coating the anode core.
[0033] A 110 gram sample of the core material was molded in a vibrated cylindrical mold
and then pressed isostatically at a pressure of about 1265 kg/cm
2 (18,000 psi) to form a cylindrical anode core having approximate dimensions of 2.75
inches by 1 inch diameter. The coating material was then molded onto the formed core
by inserting the core into a cylindrically shaped mold having larger diameter than
the core and filling the void space surrounding the core with coating material. The
coating material was compacted by vibrating. The coated core was then isostatically
pressed at a pressure of about 1406 kg/cm
2 (20,000 psi). Finally, the coating was removed from both ends of the thus-formed
body by sanding to provide both a substantially flat working surface at one end thereof
and a location for connecting the power lead to the opposite end.
[0034] The body was then sintered in oxygen at about 1420°C., using an 8 hour upheat rate
and a 4 hour hold at maximum temperature. The resistivities of the core and coating
material at 975°C. were 0.0025 ohm·cm and 0.22 ohm·cm, respectively.. The Archimedes
density of the sintered body was 95.4% of the theoretical density of 6.95 g/cm .
[0035] Densities 98% of the theoretical density have been obtained by sintering an identical
body in oxygen at 1420°C. using a 6 hour upheat rate and a 2 hour hold at maximum
temperature.
[0036] Testing of the coated monolith as an anode was conducted in a pilot scale Hall-Heroult
cell at about 980°C., the melt having the following composition:

[0037] Throughout the duration of the test, the melt was replenished periodically to maintain
approximately the starting composition. One third of the anode was immersed vertically
in the melt. After 175 hours of electrolysis at a current density of 1 amp/cm
2, the anode retained its structural integrity, exhibiting no visual sign of thermally-induced
shock or other indication of separation of the coating from the core. The uniform
appearance of the working surface of the anode coupled with the absence of corrosion
at the lower, sharp edges of the coating presented conclusive evidence that the electrolysis
current was constrained substantially to the central core region bounded by the coating.
The electrochemical corrosion of the working surface of the anode was so slight as
to not be readily capable of being quantified by physical measurements. The recorded
weight and dimensional changes of the anode were of the same order of magnitude as
the accuracy of the measurements. The coating layer exhibited high corrosion resistance
both above and below the melt level and in the region of the melt/ambient interface.
1. A non-consumable electrode suitable for use as an anode in the electrolysis of
molten salts, characterized by the fact that it is produced by the process of:
a) forming a first conductive ceramic material to produce a core having a substantially
flat working surface and a non-working surface;
b) forming a physically adherent coating over said non-working surface of said core,
on at least the portion thereof which is to be exposed to the electrolyte bath in
the cell, said coating consisting of a second conductive ceramic material having,
as compared to said first conductive ceramic material,
(1) a coefficient of thermal expansion differing by no more than about 1.0 x 10 /"C.,
(2) an essentially matched shrinkage during sintering,
(3) a higher electrical resistivity, and capable of being chemical diffusion bonded
thereto; and
c) sintering the coated core thus formed to produce a monolithic ceramic electrode
having a substantially flat working surface and a non-working surface, said non-working
surface having an impervious coating thereon, at least in the portion thereof exposed
to the electrolyte bath, of higher resistivity than the core and chemical diffusion
bonded thereto, whereby substantially all of the current applied to said electrode
is conducted into the electrolyte bath through said flat working surface.
2. A non-consumable electrode according to claim 1, characterized by the fact that
the core and the physically adherent coating are produced by isostatically pressing.
3. A non-consumable electrode according to claim 1 or 2, characterized by the fact
that the core is elongated and has two ends and the substantially flat uncoated working
surface is produced on only one end of the coated core by removing the coating therefrom.
4. A non-consumable electrode according to any one of the preceding claims, characterized
by the fact that the second conductive ceramic material has as compared to the first
conductive ceramic material, a coefficient of thermal expansion differing by no more
than about 0.5%.
5. An electrode according to any one of the preceding claims, characterized by the
fact that the core consists of 98.0-98.5 wt. % Sn02, 0.1-0.5 wt. % CuO and 1.0-1.5 wt. % Sb2O3.
6. An electrode according to any one of the preceding claims, characterized by the
fact that the coating consists of an Fe203-doped Sn02 composition.
7. An electrode according to claim 6, characterized by the fact that the coating consists
of 98.00-99.75 wt. % Sn02 and 0.25-2.00 wt. % Fe2O3.
8. A process for producing a non-consumable electrode suitable for use as an anode
in the electrolysis of molten salts, characterized by
a) forming an elongated core having two ends from a first conductive ceramic material;
b) forming a physically adherent coating over said core with a second conductive ceramic
material having, as compared to said first conductive ceramic material,
(1) a coefficient of thermal expansion differing by no more than about 1.0 x 106/°C.,
(2) an essentially matched shrinkage during sintering,
(3) a higher electrical resistivity, and capable of being chemical diffusion bonded
thereto;
cl producing a substantially flat uncoated working surface on only one end of the
coated core by removing the coating therefrom; and
d) sintering the coated core having a substantially flat uncoated working surface
to produce an integral monolithic body with an impervious coating layer,
thereby forming a ceramic electrode having a substantially flat working surface and
a non-working surface, said non-working surface having a coating of higher resistivity
than said core and chemical diffusion bonded thereto, whereby substantially all of
the current applied to said electrode is conducted into said electrode bath through
said flat working surface.
9. A process according to claim 8, characterized by the fact that the second conductive
ceramic material has, as compared to said first conductive ceramic material, a coefficient
of thermal expansion differing by no more than about 0.5%.
10. A method for manufacturing aluminum by the electrolysis of alumina in molten cryolite
in a Hall-Heroult cell characterized by the use of a non-consumable electrode according
to any one of claims 1 to 7 as the anode.