[0001] The present invention relates generally to aluminum alloys and more specifically
to a method for forming high strength aluminum alloy billets having L1
2 dispersoids therein.
[0002] The combination of high strength, ductility, and fracture toughness, as well as low
density, make aluminum alloys natural candidates for aerospace and space applications.
However, their use is typically limited to temperatures below about 300°F (149°C)
since most aluminum alloys start to lose strength in that temperature range as a result
of coarsening of strengthening precipitates.
[0003] The development of aluminum alloys with improved elevated temperature mechanical
properties is a continuing process. Some attempts have included aluminum-iron and
aluminum-chromium based alloys such as Al-Fe-Ce, Al-Fe-V-Si, Al-Fe-Ce-W, and Al-Cr-Zr-Mn
that contain incoherent dispersoids. These alloys, however, also lose strength at
elevated temperatures due to particle coarsening. In addition, these alloys exhibit
ductility and fracture toughness values lower than other commercially available aluminum
alloys.
[0004] Other attempts have included the development of mechanically alloyed Al-Mg and Al-Ti
alloys containing ceramic dispersoids. These alloys exhibit improved high temperature
strength due to the particle dispersion, but the ductility and fracture toughness
are not improved.
[0005] U.S. Patent No. 6,248,453 owned by the assignee of the present invention discloses aluminum alloys strengthened
by dispersed Al
3X L1
2 intermetallic phases where X is selected from the group consisting of Sc, Er, Lu,
Yb, Tm, and Lu. The Al
3X particles are coherent with the aluminum alloy matrix and are resistant to coarsening
at elevated temperatures. The improved mechanical properties of the disclosed dispersion
strengthened L1
2 aluminum alloys are stable up to 572°F (300°C).
U.S. Patent Application Publication No. 2006/0269437 Al also owned commonly discloses a high strength aluminum alloy that contains scandium
and other elements that is strengthened by L1
2 dispersoids.
[0006] L1
2 strengthened aluminum alloys have high strength and improved fatigue properties compared
to commercially available aluminum alloys. Fine grain size results in improved mechanical
properties of materials. Hall-Petch strengthening has been known for decades where
strength increases as grain size decreases. An optimum grain size for optimum strength
is in the nano range of about 30 to 100 nm. These alloys also have lower ductility.
[0007] The present invention is a method for forming aluminum alloy billets with high strength
and acceptable fracture toughness.
[0008] In a first aspect of the invention there is provided a method for producing high
strength aluminum alloy consolidated billets containing L1
2 dispersoids, comprising the steps of: forming an aluminum alloy powder containing
L1
2 dispersoid forming elements, wherein the L1
2 dispersoid forming elements form A1
3X dispersoids wherein X is at least one first element selected from the group comprising:
about 0.1 to about 4.0 weight percent scandium, about 0.1 to about 20.0 weight percent
erbium, about 0.1 to about 15.0 weight percent thulium, about 0.1 to about 25.0 weight
percent ytterbium, and about 0.1 to about 25.0 weight percent lutetium; at least one
second element selected from the group comprising: about 0.1 to about 20.0 weight
percent gadolinium, about 0.1 to about 20.0 weight percent yttrium, about 0.05 to
about 4.0 weight percent zirconium, about 0.05 to about 10.0 weight percent titanium,
about 0.05 to about 10.0 weight percent hafnium, and about 0.05 to about 5.0 weight
percent niobium; and the balance substantially aluminum; placing the powder in a container;
vacuum degassing the container at about 500°F (260°C) to about 900°F (482°C) for about
12 hours to about 8 days; sealing the container; creating a preform by compressing
the container by closed die forging or by quasi-isostatic forging to consolidate the
powder; encompassing the aluminum alloy powder preform with a flowable pressure transmitting
medium and heating the encompassed alloy powder; and uniaxially compressing the medium
to thereby consolidate the aluminum powder; and removing the consolidated powder billet.
[0009] In embodiments, the alloys have coherent L1
2 A1
3X dispersoids where X is at least one first element selected from scandium, erbium,
thulium, ytterbium, and lutetium, and at least one second element selected from gadolinium,
yttrium, zirconium, titanium, hafnium, and niobium. The balance is substantially aluminum
containing at least one alloying element selected from silicon, magnesium, lithium,
copper, zinc, and nickel.
[0010] The alloys are formed by encompassing a powder preform of an aluminum alloy body
containing L1
2 dispersoid forming elements in a heated, flowable pressure transmitting medium, and
rapidly compressing the powder to consolidate the perform to form the billet. Use
of graphite or a ceramic as the pressure transfer medium causes a non-isostatic pressure
field to form in the chamber. During consolidation, the powder preform undergoes an
axial compression that exceeds radial expansion. The resulting shear strain cleans
the surface oxide from the particles and increases metal-to-metal contact improving
forging density.
[0011] In a second aspect of the invention there is provided a high strength aluminum alloy
consolidated billet containing L1
2 dispersoids in an aluminum alloy matrix wherein: the L1
2 dispersoid forming elements form A1
3X dispersoids wherein X is at least one first element selected from the group comprising:
about 0.1 to about 4.0 weight percent scandium, about 0.1 to about 20.0 weight percent
erbium, about 0.1 to about 15.0 weight percent thulium, about 0.1 to about 25.0 weight
percent ytterbium, and about 0.1 to about 25.0 weight percent lutetium; at least one
second element selected from the group comprising: about 0.1 to about 20.0 weight
percent gadolinium, about 0.1 to about 20.0 weight percent yttrium, about 0.05 to
about 4.0 weight percent zirconium, about 0.05 to about 10.0 weight percent titanium,
about 0.05 to about 10.0 weight percent hafnium, and about 0.05 to about 5.0 weight
percent niobium; and the balance substantially aluminum, wherein: the aluminum alloy
consolidated billet containing L1
2 dispersoids is formed by the steps comprising: placing the powder in a container;
vacuum degassing the container at about 500°F (260°C) to about 900°F (482°C) for about
12 hours to about 8 days; sealing the container; creating a preform by compressing
the container by closed die forging or by quasi-isostatic forging to consolidate the
powder; encompassing the aluminum alloy powder preform with a flowable pressure transmitting
medium and heating the encompassed alloy powder; and uniaxially compressing the medium
to thereby consolidate the aluminum powder; and removing the consolidated powder billet.
[0013] The compression takes place in a closed container and results in billets of aluminum
alloy containing L1
2 dispersoids with a density of essentially 100%.
[0014] Certain preferred embodiments of the invention will now be described by way of example
only with reference to the accompanying drawings.
FIG. 1 is an aluminum scandium phase diagram.
FIG. 2 is an aluminum erbium phase diagram.
FIG. 3 is an aluminum thulium phase diagram.
FIG. 4 is an aluminum ytterbium phase diagram.
FIG. 5 is an aluminum lutetium phase diagram.
FIG. 6 is a schematic diagram of a vertical gas atomizer.
FIG. 7 is a scanning electron micrograph of the gas atomized inventive L12 aluminum alloy powder.
FIG. 8 is a diagram showing the processing steps to consolidate L12 aluminum alloy powder.
FIG. 9 is a schematic diagram illustrating non-isostatic forging.
FIG. 10 is a diagram showing the processing steps to Ceracon forge an L12 aluminum alloy powder preform.
1. L12 Aluminum Alloys
[0015] The alloy products of this invention are formed from aluminum based alloys with high
strength and fracture toughness for applications at temperatures from about -420°F
(-251°C) up to about 650°F (343°C). The aluminum alloy comprises a solid solution
of aluminum and at least one element selected from silicon, magnesium, lithium, copper,
zinc, and nickel strengthened by L1
2 coherent precipitates where X is at least one first element selected from scandium,
erbium, thulium, ytterbium, and lutetium, and at least one second element selected
from gadolinium, yttrium, zirconium, titanium, hafnium, and niobium.
[0016] The aluminum silicon system is a simple eutectic alloy system with a eutectic reaction
at 12.5 weight percent silicon and 1077°F (577°C). There is little solubility of silicon
in aluminum at temperatures up to 930°F (500°C) and none of aluminum in silicon. However,
the solubility can be extended significantly by utilizing rapid solidification techniques/
[0017] The binary aluminum magnesium system is a simple eutectic at 36 weight percent magnesium
and 842°F (450°C). There is complete solubility of magnesium and aluminum in the rapidly
solidified inventive alloys discussed herein.
[0018] The binary aluminum lithium system is a simple eutectic at 8 weight percent lithium
and 1105°F (596°C). The equilibrium solubility of 4 weight percent lithium can be
extended significantly by rapid solidification techniques. There can be complete solubility
of lithium in the rapid solidified inventive alloys discussed herein.
[0019] The binary aluminum copper system is a simple eutectic at 32 weight percent copper
and 1018°F (548°C). There can be complete solubility of copper in the rapidly solidified
inventive alloys discussed herein.
[0020] The aluminum zinc binary system is a eutectic alloy system involving a monotectoid
reaction and a miscibility gap in the solid state. There is a eutectic reaction at
94 weight percent zinc and 718°F (381°C). Zinc has maximum solid solubility of 83.1
I weight percent in aluminum at 717.8°F (381°C) which can be extended by rapid solidification
processes. Decomposition of the super saturated solid solution of zinc in aluminum
gives rise to spherical and ellipsoidal GP zones which are coherent with the matrix
and act to strengthen the alloy.
[0021] The aluminum nickel binary system is a simple eutectic at 5.7 weight percent nickel
and 1183.8°F (639.9°C). There is little solubility of nickel in aluminum. However,
the solubility can be extended significantly by utilizing rapid solidification processes.
The equilibrium phase in the aluminum nickel eutectic system is L1
2 intermetallic A1
3Ni.
[0022] In the aluminum based alloys disclosed herein, scandium, erbium, thulium, ytterbium,
and lutetium are potent strengtheners that have low diffusivity and low solubility
in aluminum. All these elements form equilibrium A1
3X intermetallic dispersoids where X is at least one of scandium, erbium, thulium,
ytterbium, and lutetium, that have an L1
2 structure that is an ordered face centered cubic structure with the X atoms located
at the corners and aluminum atoms located on the cube faces of the unit cell.
[0023] Scandium forms Al
3Sc dispersoids that are fine and coherent with the aluminum matrix. Lattice parameters
of aluminum and Al
3Sc are very close (0.405 nm and 0.410 nm respectively), indicating that there is minimal
or no driving force for causing growth of the Al
3Sc dispersoids. This low interfacial energy makes the Al
3Sc dispersoids thermally stable and resistant to coarsening up to temperatures as
high as about 842°F (450°C). Additions of magnesium in aluminum increase the lattice
parameter of the aluminum matrix, and decrease the lattice parameter mismatch further
increasing the resistance of the Al
3Sc to coarsening. Additions of zinc, copper, lithium, silicon, and nickel provide
solid solution and precipitation strengthening in the aluminum alloys. In the alloys
of this invention these Al
3Sc dispersoids are made stronger and more resistant to coarsening at elevated temperatures
by adding suitable alloying elements such as gadolinium, yttrium, zirconium, titanium,
hafnium, niobium, or combinations thereof, that enter Al
3Sc in solution.
[0024] Erbium forms A1
3Er dispersoids in the aluminum matrix that are fine and coherent with the aluminum
matrix. The lattice parameters of aluminum and A1
3Er are close (0.405 nm and 0.417 nm respectively), indicating there is minimal driving
force for causing growth of the A1
3Er dispersoids. This low interfacial energy makes the A1
3Er dispersoids thermally stable and resistant to coarsening up to temperatures as
high as about 842°F (450°C). Additions of magnesium in aluminum increase the lattice
parameter of the aluminum matrix, and decrease the lattice parameter mismatch further
increasing the resistance of the A1
3Er to coarsening. Additions of zinc, copper, lithium, silicon, and nickel provide
solid solution and precipitation strengthening in the aluminum alloys. In the alloys
of this invention, these Al
3Er dispersoids are made stronger and more resistant to coarsening at elevated temperatures
by adding suitable alloying elements such as gadolinium, yttrium, zirconium, titanium,
hafnium, niobium, or combinations thereof that enter Al
3Er in solution.
[0025] Thulium forms metastable Al
3Tm dispersoids in the aluminum matrix that are fine and coherent with the aluminum
matrix. The lattice parameters of aluminum and Al
3Tm are close (0.405 nm and 0.420 nm respectively), indicating there is minimal driving
force for causing growth of the Al
3Tm dispersoids. This low interfacial energy makes the Al
3Tm dispersoids thermally stable and resistant to coarsening up to temperatures as
high as about 842°F (450°C). Additions of magnesium in aluminum increase the lattice
parameter of the aluminum matrix, and decrease the lattice parameter mismatch further
increasing the resistance of the Al
3Tm to coarsening. Additions of zinc, copper, lithium, silicon, and nickel provide
solid solution and precipitation strengthening in the aluminum alloys. In the alloys
of this invention these Al
3Tm dispersoids are made stronger and more resistant to coarsening at elevated temperatures
by adding suitable alloying elements such as gadolinium, yttrium, zirconium, titanium,
hafnium, niobium, or combinations thereof that enter Al
3Tm in solution.
[0026] Ytterbium forms Al
3Yb dispersoids in the aluminum matrix that are fine and coherent with the aluminum
matrix. The lattice parameters of Al and A1
3Yb are close (0.405 nm and 0.420 nm respectively), indicating there is minimal driving
force for causing growth of the A1
3Yb dispersoids. This low interfacial energy makes the A1
3Yb dispersoids thermally stable and resistant to coarsening up to temperatures as
high as about 842°F (450°C). Additions of magnesium in aluminum increase the lattice
parameter of the aluminum matrix, and decrease the lattice parameter mismatch further
increasing the resistance of the Al
3Yb to coarsening. Additions of zinc, copper, lithium, silicon, and nickel provide
solid solution and precipitation strengthening in the aluminum alloys. In the alloys
of this invention, these Al
3Yb dispersoids are made stronger and more resistant to coarsening at elevated temperatures
by adding suitable alloying elements such as gadolinium, yttrium, zirconium, titanium,
hafnium, niobium, or combinations thereof that enter Al
3Yb in solution.
[0027] Lutetium forms Al
3Lu dispersoids in the aluminum matrix that are fine and coherent with the aluminum
matrix. The lattice parameters of Al and Al
3Lu are close (0.405 nm and 0.419 nm respectively), indicating there is minimal driving
force for causing growth of the Al
3Lu dispersoids. This low interfacial energy makes the Al
3Lu dispersoids thermally stable and resistant to coarsening up to temperatures as
high as about 842°F (450°C). Additions of magnesium in aluminum increase the lattice
parameter of the aluminum matrix, and decrease the lattice parameter mismatch further
increasing the resistance of the Al
3Lu to coarsening. Additions of zinc, copper, lithium, silicon, and nickel provide
solid solution and precipitation strengthening in the aluminum alloys. In the alloys
of this invention, these Al
3Lu dispersoids are made stronger and more resistant to coarsening at elevated temperatures
by adding suitable alloying elements such as gadolinium, yttrium, zirconium, titanium,
hafnium, niobium, or mixtures thereof that enter Al
3Lu in solution.
[0028] Gadolinium forms metastable Al
3Gd dispersoids in the aluminum matrix that are stable up to temperatures as high as
about 842°F (450°C) due to their low diffusivity in aluminum. The Al
3Gd dispersoids have a D0
19 structure in the equilibrium condition. Despite its large atomic size, gadolinium
has fairly high solubility in the Al
3X intermetallic dispersoids (where X is.scandium, erbium, thulium, ytterbium or lutetium).
Gadolinium can substitute for the X atoms in Al
3X intermetallic, thereby forming an ordered L1
2 phase which results in improved thermal and structural stability.
[0029] Yttrium forms metastable Al
3Y dispersoids in the aluminum matrix that have an L1
2 structure in the metastable condition and a D0
19 structure in the equilibrium condition. The metastable Al
3Y dispersoids have a low diffusion coefficient which makes them thermally stable and
highly resistant to coarsening. Yttrium has a high solubility in the Al
3X intermetallic dispersoids allowing large amounts of yttrium to substitute for X
in the Al
3X L1
2 dispersoids which results in improved thermal and structural stability.
[0030] Zirconium forms Al
3Zr dispersoids in the aluminum matrix that have an L1
2 structure in the metastable condition and D0
23 structure in the equilibrium condition. The metastable Al
3Zr dispersoids have a low diffusion coefficient which makes them thermally stable
and highly resistant to coarsening. Zirconium has a high solubility in the Al
3X dispersoids allowing large amounts of zirconium to substitute for X in the Al
3X dispersoids, which results in improved thermal and structural stability.
[0031] Titanium forms Al
3Ti dispersoids in the aluminum matrix that have an L1
2 structure in the metastable condition and DO
22 structure in the equilibrium condition. The metastable Al
3Ti despersoids have a low diffusion coefficient which makes them thermally stable
and highly resistant to coarsening. Titanium has a high solubility in the Al
3X dispersoids allowing large amounts of titanium to substitute for X in the Al
3X dispersoids, which result in improved thermal and structural stability.
[0032] Hafnium forms metastable Al
3 Hf dispersoids in the aluminum matrix that have an L1
2 structure in the metastable condition and a D0
23 structure in the equilibrium condition. The Al
3Hf dispersoids have a low diffusion coefficient, which makes them thermally stable
and highly resistant to coarsening. Hafnium has a high solubility in the Al
3X dispersoids allowing large amounts of hafnium to substitute for scandium, erbium,
thulium, ytterbium, and lutetium in the above mentioned Al
3X dispersoids, which results in stronger and more thermally stable dispersoids.
[0033] Niobium forms metastable Al
3Nb dispersoids in the aluminum matrix that have an L1
2 structure in the metastable condition and a D0
22 structure in the equilibrium condition. Niobium has a lower solubility in the A1
3X dispersoids than hafnium or yttrium, allowing relatively lower amounts of niobium
than hafnium or yttrium to substitute for X in the A1
3X dispersoids. Nonetheless, niobium can be very effective in slowing down the coarsening
kinetics of the A1
3X dispersoids because the Al
3Nb dispersoids are thermally stable. The substitution of niobium for X in the above
mentioned Al
3X dispersoids results in stronger and more thermally stable dispersoids.
[0034] Al
3X L1
2 precipitates improve elevated temperature mechanical properties in aluminum alloys
for two reasons. First, the precipitates are ordered intermetallic compounds. As a
result, when the particles are sheared by glide dislocations during deformation, the
dislocations separate into two partial dislocations separated by an anti-phase boundary
on the glide plane. The energy to create the anti-phase boundary is the origin of
the strengthening. Second, the cubic L1
2 crystal structure and lattice parameter of the precipitates are closely matched to
the aluminum solid solution matrix. This results in a lattice coherency at the precipitate/matrix
boundary that resists coarsening. The lack of an interphase boundary results in a
low driving force for particle growth and resulting elevated temperature stability.
Alloying elements in solid solution in the dispersed strengthening particles and in
the aluminum matrix that tend to decrease the lattice mismatch between the matrix
and particles will tend to increase the strengthening and elevated temperature stability
of the alloy.
[0035] L1
2 phase strengthened aluminum alloys are important structural materials because of
their excellent mechanical properties and the stability of these properties at elevated
temperature due to the resistance of the coherent dispersoids in the microstructure
to particle coarsening. The mechanical properties are optimized by maintaining a high
volume fraction of L1
2 dispersoids in the microstructure. The L1
2 dispersoid concentration following aging scales as the amount of L1
2 phase forming elements in solid solution in the aluminum alloy following quenching.
Examples of L1
2 phase forming elements include but are not limited to Sc, Er, Th, Yb, and Lu. The
concentration of alloying elements in solid solution in alloys cooled from the melt
is directly proportional to the cooling rate.
[0036] Exemplary aluminum alloys for the bimodal system alloys of this invention include,
but are not limited to (in weight percent unless otherwise specified):
about Al-M-(0.1-4)Sc-(0.1-20)Gd;
about Al-M-(0.1-20)Er-(0.1-20)Gd;
about Al-M-(0.1-15)Tm-(0.1-20)Gd;
about Al-M-(0.1-25)Yb-(0.1-20)Gd;
about Al-M-(0.1-25)Lu-(0.1-20)Gd;
about Al-M-(0.1-4)Sc-(0.1-20)Y;
about Al-M-(0.1-20)Er-(0.1-20)Y;
about Al-M-(0.1-15)Tm-(0.1-20)Y;
about Al-M-(0.1-25)Yb-(0.1-20)Y;
about Al-M-(0.1-25)Lu-(0.1-20)Y;
about Al-M-(0.1-4)Sc-(0.05-4)Zr;
about Al-M-(0.1-20)Er-(0.05-4)Zr;
about Al-M-(0.1-15)Tm-(0.054)Zr;
about Al-M-(0.1-25)Yb-(0.05-4)Zr;
about Al-M-(0.1-25)Lu-(0.05-4)Zr;
about Al-M-(0.1-4)Sc-(0.05-10)Ti;
about Al-M-(0.1-20)Er-(0.05-10)Ti;
about Al-M-(0.1-15)Tm-(0.05-10)Ti;
about Al-M- (0.1-25)Yb-(0.05-10)Ti;
about Al-M-(0.1-25)Lu-(0.05-10)Ti;
about Al-M-(0.1-4)Sc-(0.05-10)Hf;
about Al-M-(0.1-20)Er-(0.05-10)Hf;
about Al-M-(0.1-15)Tm-(0.05-10)Hf;
about Al-M-(0.1-25)Yb-(0.05-10)Hf;
about Al-M-(0.1-25)Lu-(0.05-10)Hf;
about Al-M-(0.1-4)Sc-(0.05-5)Nb;
about Al-M-(0.1-20)Er-(0.05-5)Nb;
about Al-M-(0.1-15)Tm-(0.05-5)Nb;
about Al-M-(0.1-25)Yb-(0.05-5)Nb; and
about Al-M-(0.1-25)Lu-(0.05-5)Nb.
[0037] M is at least one of about (4-25) weight percent silicon, (1-8) weight percent magnesium,
(0.5-3) weight percent lithium, (0.2-6.5) weight percent copper, (3-12) weight percent
zinc, and (1-12) weight percent nickel.
[0038] The amount of silicon present in the fine grain matrix of this invention if any may
vary from about 4 to about 25 weight percent, more preferably from about 4 to about
18 weight percent, and even more preferably from about 5 to about 11 weight percent.
[0039] The amount of magnesium present in the fine grain matrix of this invention if any
may vary from about 1 to about 8 weight percent, more preferably from about 3 to about
7.5 weight percent, and even more preferably from about 4 to about 6.5 weight percent.
[0040] The amount of lithium present in the fine grain matrix of this invention if any may
vary from about 0.5 to about 3 weight percent, more preferably from about 1 to about
2.5 weight percent, and even more preferably from about 1 to about 2 weight percent.
[0041] The amount of copper present in the fine grain matrix of this invention if any may
vary from about 0.2 to about 6.5 weight percent, more preferably from about 0.5 to
about 5.0 weight percent, and even more preferably from about 2 to about 4.5 weight
percent.
[0042] The amount of zinc present in the fine grain matrix of this invention if any may
vary from about 3 to about 12 weight percent, more preferably from about 4 to about
10 weight percent, and even more preferably from about 5 to about 9 weight percent.
[0043] The amount of nickel present in the fine grain matrix of this invention if any may
vary from about 1 to about 12 weight percent, more preferably from about 2 to about
10 weight percent, and even more preferably from about 4 to about 10 weight percent.
[0044] The amount of scandium present in the fine grain matrix of this invention if any
may vary from 0.1 to about 4 weight percent, more preferably from about 0.1 to about
3 weight percent, and even more preferably from about 0.2 to about 2.5 weight percent.
The Al-Sc phase diagram shown in FIG. 1 indicates a eutectic reaction at about 0.5
weight percent scandium at about 1219°F (659°C) resulting in a solid solution of scandium
and aluminum and Al
3Sc dispersoids. Aluminum alloys with less than 0.5 weight percent scandium can be
quenched from the melt to retain scandium in solid solution that may precipitate as
dispersed L1
2 intermetallic Al
3Sc following an aging treatment. Alloys with scandium in excess of the eutectic composition
(hypereutectic alloys) can only retain scandium in solid solution by rapid solidification
processing (RSP) where cooling rates are in excess of about 10
3°C/second.
[0045] The amount of erbium present in the fine grain matrix of this invention, if any,
may vary from about 0.1 to about 20 weight percent, more preferably from about 0.3
to about 15 weight percent, and even more preferably from about 0.5 to about 10 weight
percent. The Al-Er phase diagram shown in FIG. 2 indicates a eutectic reaction at
about 6 weight percent erbium at about 1211°F (655°C). Aluminum alloys with less than
about 6 weight percent erbium can be quenched from the melt to retain erbium in solid
solutions that may precipitate as dispersed L1
2 intermetallic Al
3Er following an aging treatment. Alloys with erbium in excess of the eutectic composition
can only retain erbium in solid solution by rapid solidification processing (RSP)
where cooling rates are in excess of about 10
3°C/second.
[0046] The amount of thulium present in the alloys of this invention, if any, may vary from
about 0.1 to about 15 weight percent, more preferably from about 0.2 to about 10 weight
percent, and even more preferably from about 0.4 to about 6 weight percent. The Al-Tm
phase diagram shown in FIG. 3 indicates a eutectic reaction at about 10 weight percent
thulium at about 1193°F (645°C). Thulium forms metastable Al
3Tm dispersoids in the aluminum matrix that have an L1
2 structure in the equilibrium condition. The Al
3Tm dispersoids have a low diffusion coefficient which makes them thermally stable
and highly resistant to coarsening. Aluminum alloys with less than 10 weight percent
thulium can be quenched from the melt to retain thulium in solid solution that may
precipitate as dispersed metastable L1
2 intermetallic Al
3Tm following an aging treatment. Alloys with thulium in excess of the eutectic composition
can only retain Tm in solid solution by rapid solidification processing (RSP) where
cooling rates are in excess of about 10
3°C/second.
[0047] The amount of ytterbium present in the alloys of this invention, if any, may vary
from about 0.1 to about 25 weight percent, more preferably from about 0.3 to about
20 weight percent, and even more preferably from about 0.4 to about 10 weight percent.
The Al-Yb phase diagram shown in FIG. 4 indicates a eutectic reaction at about 21
weight percent ytterbium at about 1157°F (625°C). Aluminum alloys with less than about
21 weight percent ytterbium can be quenched from the melt to retain ytterbium in solid
solution that may precipitate as dispersed L1
2 intermetallic A1
3Yb following an aging treatment. Alloys with ytterbium in excess of the eutectic composition
can only retain ytterbium in solid solution by rapid solidification processing (RSP)
where cooling rates are in excess of about 10
3°C/second.
[0048] The amount of lutetium present in the alloys of this invention, if any, may vary
from about 0.1 to about 25 weight percent, more preferably from about 0.3 to about
20 weight percent, and even more preferably from about 0.4 to about 10 weight percent.
The Al-Lu phase diagram shown in FIG. 5 indicates a eutectic reaction at about 11.7
weight percent Lu at about 1202°F (650°C). Aluminum alloys with less than about 11.7
weight percent lutetium can be quenched from the melt to retain Lu in solid solution
that may precipitate as dispersed L1
2 intermetallic Al
3Lu following an aging treatment. Alloys with Lu in excess of the eutectic composition
can only retain Lu in solid solution by rapid solidification processing (RSP) where
cooling rates are in excess of about 10
3°C/second.
[0049] The amount of gadolinium present in the alloys of this invention, if any, may vary
from about 0.1 to about 20 weight percent, more preferably from about 0.3 to about
15 weight percent, and even more preferably from about 0.5 to about 10 weight percent.
[0050] The amount of yttrium present in the alloys of this invention, if any, may vary from
about 0.1 to about 20 weight percent, more preferably from about 0.3 to about 15 weight
percent, and even more preferably from about 0.5 to about 10 weight percent.
[0051] The amount of zirconium present in the alloys of this invention, if any, may vary
from about 0.05 to about 4 weight percent, more preferably from about 0.1 to about
3 weight percent, and even more preferably from about 0.3 to about 2 weight percent.
[0052] The amount of titanium present in the alloys of this invention, if any, may vary
from about 0.05 to about 10 weight percent, more preferably from about 0.2 to about
8 weight percent, and even more preferably from about 0.4 to about 4 weight percent.
[0053] The amount of hafnium present in the alloys of this invention, if any, may vary from
about 0.05 to about 10 weight percent, more preferably from about 0.2 to about 8 weight
percent, and even more preferably from about 0.4 to about 5 weight percent.
[0054] The amount of niobium present in the alloys of this invention, if any, may vary from
about 0.05 to about 5 weight percent, more preferably from about 0.1 to about 3 weight
percent, and even more preferably from about 0.2 to about 2 weight percent.
[0055] In order to have the best properties for the fine grain matrix of this invention,
it is desirable to limit the amount of other elements. Specific elements that should
be reduced or eliminated include no more than about 0.1 weight percent iron, 0.1 weight
percent chromium, 0.1 weight percent manganese, 0.1 weight percent vanadium, and 0.1
weight percent cobalt. The total quantity of additional elements should not exceed
about 1% by weight, including the above listed impurities and other elements.
2. Ceracon Forging of L12 Aluminum Alloys
[0056] It is advantageous to form L1
2 strengthened aluminum alloy product from powder. The major reason is that the rapid
cooling rate experienced during powder formation from the melt results in high supersaturation
of intermetallic L1
2 phase forming elements in the powder. The high supersaturation leads to a maximum
amount of the strengthening phase dispersed throughout the structure in the final
consolidated part.
[0057] The highest cooling rates observed in commercially viable processes are achieved
by gas atomization of molten metals to produce powder. Gas atomization is a two fluid
process wherein a stream of molten metal is disintegrated by a high velocity gas stream.
The end result is that the particles of molten metal eventually become spherical due
to surface tension and finely solidify in powder form. Heat from the liquid droplets
is transferred to the atomization gas by convection. The solidification rates, depending
on the gas and the surrounding environment, can be very high and can exceed 10
6°C/second. Cooling rates greater than 10
3°C/second are typically specified to ensure supersaturation of alloying elements in
gas atomized L1
2 aluminum alloy powder in the inventive process described herein.
[0058] A schematic of typical vertical gas atomizer 100 is shown in FIG. 6A. FIG. 6A is
taken from
R. Germain, Powder Metallurgy Science Second Edition MPIF (1994) (chapter 3, p. 101) and is incorporated herein by reference. Vacuum or inert gas induction melter 102
is positioned at the top of free flight chamber 104. Vacuum induction melter 102 contains
melt 106 which flows by gravity or gas overpressure through nozzle 108. A close up
view of nozzle 108 is shown in FIG. 6B. Melt 106 enters nozzle 108 and flows downward
till it meets high pressure gas stream from gas source 110 where it is transformed
into a spray of droplets. The droplets eventually become spherical due to surface
tension and rapidly solidify into spherical powder 112 which collects in collection
chamber 114. The gas recirculates through cyclone collector 116 which collects fine
powder 118 before returning to the input gas stream. As can be seen from FIG. 6A,
the surroundings to which the melt and eventual powder are exposed are completely
controlled.
[0059] There are many effective nozzle designs known in the art to produce spherical metal
powder. Nozzle designs with short gas-to-melt separation distances produce finer powders.
Confined nozzle designs where gas meets the molten stream at a short distance just
after it leaves the atomization nozzle are preferred for the production of the inventive
L1
2 aluminum alloy powders disclosed herein. Higher superheat temperatures cause lower
melt viscosity and longer cooling times. Both result in smaller spherical particles.
[0060] A large number of processing parameters are associated with gas atomization that
affect the final product. Examples include melt superheat, gas pressure, metal flow
rate, gas type, and gas purity. In gas atomization, the particle size is related to
the energy input to the metal. Higher gas pressures, higher superheat temperatures
and lower metal flow rates result in smaller particle sizes. Higher gas pressures
provide higher gas velocities for a given atomization nozzle design.
[0061] To maintain purity, inert gases are used, such as helium, argon, and nitrogen. Helium
is preferred for rapid solidification because the high heat transfer coefficient of
the gas leads to high quenching rates and high supersaturation of alloying elements.
[0062] Lower metal flow rates and higher gas flow rates favor production of finer powders.
The particle size of gas atomized melts typically has a log normal distribution. An
example of spherical L1
2 aluminum alloy powder is shown in the scanning electron micrograph (SEM) of FIG.
7.
[0063] Oxygen and hydrogen in the powder can degrade the mechanical properties of the final
part. It is preferred to limit the oxygen in the L1
2 alloy powder to about 1 ppm to 2000 ppm. Oxygen is intentionally introduced as a
component of the helium gas during atomization. A thin oxide coating on the L1
2 aluminum powder is beneficial for two reasons. First, the coating prevents agglomeration
by contact sintering and secondly, the coating inhibits the chance of explosion of
the powder. A controlled amount of oxygen is important in order to provide good ductility
and fracture toughness in the final consolidated material. Hydrogen content in the
powder is controlled by ensuring the dew point of the helium gas is low. A dew point
of about minus 50°F (minus 45.5°C) to minus 100°F (minus 73.3°C) is preferred.
[0064] In preparation for final processing, the powder is classified according to size by
sieving. To prepare the powder for sieving, if the powder has zero percent oxygen
content, the powder may be exposed to nitrogen gas which passivates the powder surface
and prevents agglomeration. Finer powder sizes result in improved mechanical properties
of the end product. While minus 325 mesh (about 45 microns) powder can be used, minus.
450 mesh (about 30 microns) powder is a preferred size in order to provide good mechanical
properties in the end product. During the atomization process, powder is collected
in collection chambers in order to prevent oxidation of the powder. Collection chambers
are used at the bottom of atomization chamber 104 as well as at the bottom of cyclone
collector 116. The powder is transported and stored in the collection chambers also.
Collection chambers are maintained under positive pressure with nitrogen gas which
prevents oxidation of the powder.
[0065] The process of consolidating the inventive alloy powders into useful forms is schematically
illustrated in FIG. 8. L1
2 aluminum alloy powders 210 are first classified according to size by sieving (step
220). Fine particle sizes are required for optimum mechanical properties in the final
part. Next, the classified powders are blended (step 230) in order to maintain microstructural
homogeneity in the final part. Blending is necessary because different atomization
batches produce powders with varying particle size distributions. Other benefits of
blending will be discussed later. Powders may be optionally cryomilled (step 240)
to minimize grain size and improve strength. Cryomilling is carried out in a high-energy
ball mill under liquid nitrogen, and offers several benefits that will be discussed
later.
[0066] The sieved, blended and (optionally) cryomilled powders are then put in a can (step
250) and vacuum degassed (step 260). Following vacuum degassing, the can is sealed
(step 270) under vacuum and forged (step 280) to produce a densified preform. Finally,
the preform is Ceracon forged (step 290) to produce a product with improved mechanical
properties useful for subsequent service as a high temperature L1
2 strengthened aluminum alloy. Non-isostatic Ceracon forging will be described later.
[0067] Sieving (step 220) is a critical step in consolidation because the final mechanical
properties relate directly to the particle size. Finer particle size results in finer
L1
2 particle dispersion and finer grain size. Optimum mechanical properties have been
observed with -450 mesh (30 micron) powder. Sieving (step 220) also limits the defect
size in the powder. Before sieving, the powder is passivated with nitrogen gas in
order to prevent agglomeration. Ultrasonic sieving is preferred for its efficiency.
[0068] Blending (step 230) is another critical step in the consolidation process because
it results in improved uniformity of particle size distribution. Gas atomized L1
2 aluminum alloy powder generally exhibits a bimodal particle size distribution and
cross blending of separate powder batches tends to homogenize the particle size distribution.
Blending (step 230) is also necessary when separate metal and/or ceramic powders are
added to the L1
2 base powder to form bimodal and trimodal consolidated alloy microstructures.
[0069] Cryomilling (step 240) can be used to refine the grain size of gas atomized L1
2 aluminum alloy powder as well as the final consolidated alloy microstructure. Cryomilling
is described in
U.S. Patent No. 6,902,699, Fritzemeier et al. and in
U.S. Patent No. 7,344,675, Van Daam et al. and are incorporated herein in their entirety by reference. Cryomilling involves
high-energy ball milling under liquid nitrogen. The liquid nitrogen environment prevents
oxidation and prevents frictional heating of the powder and the resulting grain coarsening.
During the process, the powder particles are repeatedly sheared, fractured and cold
welded which results in a severely deformed microstructure containing a high dislocation
density that, with continued deformation, evolves into a cellular structure consisting
of extremely small dislocation free grains separated by high angle grain boundaries
with high dislocation density. The grain size of the cellular microstructure is typically
less than 100 nm and the microstructure is considered a nanostructure.
[0070] In addition, the nitrogen environment results in the formation of nitride particles
that reside at the grain boundaries and in the grain interiors and resist coarsening
at higher temperatures. Stearic acid is preferably added to the powder charge to prevent
excessive agglomeration and to promote fracturing and rewelding of the L1
2 aluminum alloy particles during milling.
[0071] Following sieving (step 220), blending (step 230) and (optionally) cryomilling (Step
240), the powders are transferred to a can (step 250) where the powder is vacuum degassed
(step 260) for about 12 hours to over 8 days at elevated temperatures. A temperature
range of about 500°F (260°C) to about 900°F (482°C) is preferred and about 750°F (399°C)
is more preferred. Dynamic degassing large amounts of powder are preferred to static
degassing to expose all of the powder to a uniform temperature. Degassing removes
the stearic acid lubricant as well as oxygen and hydrogen from the charge.
[0072] Following vacuum degassing (step 260), the vacuum line is crimped and welded shut.
The powder is then consolidated into a dense preform by closed die forging or by quasi-isostatic
forging (step 280).
[0073] An exemplary embodiment of this invention is to consolidate a canned L1
2 aluminum alloy powder preform into a substantially 100% dense billet by a quasi-isostatic
Ceracon-type forging process. The forging process consists of uniaxially pressing
the canned powder preform or solid part perform in a cylindrical press, wherein the
preform is surrounded by pressure transmitting medium during the forging. A schematic
of quasi-isostatic forging equipment 300 is shown in FIG. 9. The equipment consists
of cylindrical die 310 on base 320 with ram 325 inserted in dye cavity 330. Quasi-isostatic
forging is carried out at elevated temperatures schematically illustrated by heating
coils 340.
[0074] The steps to Ceracon forge an L1
2 aluminum alloy powder preform are schematically illustrated in FIG. 10. First die
310 is (optionally) preheated (step 410). The preheat temperature is preferably about
40°F (4.5°C) to about 70°F (21°C) higher than the forging temperature to compensate
for cooling that occurs during the loading process. Next, die 310 is partially filled
with pressure transmitting medium (PTM) 360 (step 420). To minimize cooling during
loading, the PTM can be (optionally) preheated, preferably to the same temperature
as the die (step 450). Consolidated powder preform 350 is then inserted in die 310.
Powder preform 350 can be (optionally) preheated, preferably to the same temperature
as die 310 and PTM 360 (step 440). The remainder of die cavity 330 is then filled
with PTM 360 (step 460). PTM 360 can be (optionally) heated (step 450). Ram 325 is
then inserted in die 310 (step 470). Pressure 370 is applied to Ram 325 to accomplish
quasi-isostatic Ceracon type forging.
[0075] One advantage of this process is that, if the preheating steps are followed, the
run time is short. As a result, deleterious microstructural changes, such as grain
and particle coarsening are minimized. Run times can be as short as a few minutes
if automated loading and charging equipment is used. In addition, ductility and fracture
toughness of L1
2 based aluminum alloys can be improved significantly due to dynamic bimodal pressure
generated during quasi-isostatic forging that breaks apart continuous powder surface
oxide that prevent metal-metal bonding and randomly distributes them in the material.
[0076] During quasi-isostatic Ceracon type forging, the billet axially deforms about 30%
and radially deforms about 10%. Strain rates from about 0.1 min
-1 to about 6 min
-1 at forging temperatures from about 400°F (204°C) to about 900°F (482°C) are preferred.
Forging pressures from 50 ksi (345 MPa) to 150 ksi (1034 MPa) are preferred.
[0077] The pressure transmitting medium can consist of graphite or other carbon containing
powders or ceramic powders or both. By proper fixturing and preheating the pressure
transmitting medium and the work piece, densification during quasi-isostatic forging
can be extremely rapid on the order of minutes.
[0078] The unequal actual and radial deformation of the powder is schematically illustrated
by the dotted line outline of deformed can 352 in FIG. 9.
[0079] Quasi-isostatic forging of a 60 to 80 percent dense aluminum-7.5 weight percent magnesium
powder preform by this technique resulted in about a 30 percent axial compression
and about a 10 percent radial expansion as taught by
Meeks III et al. U.S. Patent No. 7,097,807 and included herein by reference. The quasi-isostatic forging deformation of L1
2 aluminum alloy powder of this embodiment has beneficial effects on the microstructure
and resulting properties of the consolidated billet. The nonuniform stress and resulting
strain field in the powder during forging results in extensive shear deformation.
The shear deformation deforms the powder, strips off the surface oxide from the L1
2 alloy particles and redistributes it throughout the consolidated L1
2 aluminum alloy powder forging as finely divided dispersoids. As a result, there is
increased metal to metal contact during forging and resulting increased mechanical
integrity. The redistributed surface oxide particles act as additional strengthening
agents by resisting dislocation motion by Orowan strengthening.
[0080] In other embodiments, Ceracon type forging can be followed by hot isostatic pressing
(HIP), forging, rolling and other deformation processing techniques.
[0081] To summarize, Ceracon type quasi-isostatic forging can be low cost and efficient.
The pressure transmitting medium, as well as the vacuum sealed preform can be preheated
prior to introduction of the perform into the forging chamber to minimize runtime.
In addition, forging can be accomplished at high strain rates resulting in forging
runs lasting less than a few minutes. The short run time results in an economical
process that also further inhibits grain and L1
2 particle growth in the billet during forging due to the limited time at temperature.
The pressure transmitting medium can be reused and loading and unloading the preforms
and resulting forgings can be an automated procedure.
[0082] Although the present invention has been described with reference to preferred embodiments,
workers skilled in the art will recognize that changes may be made in form and detail
without departing from the scope of the invention which is defined by the attached
claims.
[0083] In at least a preferred embodiment of the invention there is provided a high strength
aluminum alloy consolidated billet containing L1
2 dispersoids in an aluminum alloy matrix wherein: the L1
2 dispersoid forming elements form A1
3X dispersoids wherein X is at least one first element selected from the group comprising:
about 0.1 to about; 4.0 weight percent scandium, about 0.1 to about 20.0 weight percent
erbium, about 0.1 to about 15.0 weight percent thulium, about 0.1 to about 25.0 weight
percent ytterbium, and about 0.1 to about 25.0 weight percent lutetium; at least one
second element selected from the group comprising: about 0.1 to about 20.0 weight
percent gadolinium, about 0.1 to about 20.0 weight percent yttrium, about 0.05 to
about 4.0 weight percent zirconium, about 0.05 to about 10.0 weight percent titanium,
about 0.05 to about 10.0 weight percent hafnium, and about 0.05 to about 5.0 weight
percent niobium; and the balance substantially aluminum, wherein: the aluminum alloy
consolidated billet containing L1
2 dispersoids is formed by the steps comprising: placing the powder in a container;
vacuum degassing the container at about 500°F (260°C) to about 900°F (482°C) for about
12 hours to about 8 days; sealing the container; creating a preform by compressing
the container by closed die forging or by quasi-isostatic forging to consolidate the
powder; encompassing the aluminum alloy powder preform with a flowable pressure transmitting
medium and heating the encompassed alloy powder and medium; and uniaxially compressing
the medium at an axial strain rate of from about 0.1 min
-1 to about 6 min
-1 at a pressure from about 50 KSi (345 MPa) to about 150 KSi (1034 MPa) to thereby
consolidate the aluminum powder; and removing the consolidated powder in a billet.