[0001] Lower cost high strength single crystal superalloys with reduced rhenium and ruthenium
content are described.
[0002] All second and higher generation nickel-base directionally solidified and single
crystal superalloy compositions contain additions of rhenium of at least 3 wt%. Fourth
generation and higher single crystal alloys contain some percentage of the element
ruthenium. With the significant escalation of spot prices of these elements, there
is an economic need for alternate alloy compositions with comparable levels of performance,
but with reduced concentration of these expensive elements.
[0003] Nickel-base superalloy single crystals are primarily used for high temperature turbine
components, such as blades and vanes, where temperature capability is typically assessed
by its high temperature creep resistance. Simplistically, it is well understood that
to improve creep resistance, additions of refractory elements with high melting point
is desirable. Such elements include almost all Group IVA to VIIIA transition metals,
especially Ti, Nb, Ta, Mo, W, Re, and Ru with melting points in excess of 4082°F (2250°C).
Among these elements, Ti, Nb, and Ta are known to almost exclusively replace Al in
the ordered precipitate phase γ'(Ni
3Al), whereas Re and Ru are known to exclusively partition to the nickel base solid
solution γ-matrix. W on the other hand is known to partition evenly between the γ-matrix
and γ'
, phase.
[0004] There are of course limits to the extent to which these elements can be accommodated
in the alloy. It is common knowledge that optimum mechanical properties are obtained
when the volume fraction of the γ' phase is around 60 to 70%. Thus, individually or
combined (Al + Nb + Ta + W/2) in atom % cannot exceed about 18%. Moreover, Al concentrations
cannot be reduced below 10 atom% to preserve oxidation resistance. Similarly excessive
addition of refractory elements in the γ-matrix is limited by the undesirable phases
these elements can form after a long time exposure. The formation of so-called topologically
closed packed (TCP) phases are undesirable as they reduce the creep resistance of
the alloy. The concentration at which such phases will form can be approximately predicted
by calculating, what is called an electron vacancy number or Nv number for the γ-matrix.
This calculation is based on a weighed average of Nv assigned to each element. It
is an industry wide practice to use such calculations, but it is known that it is
not completely accurate and there are exceptions to the rule.
[0005] There is a need for a lower cost high strength nickel based superalloy.
[0006] Thus according to a first aspect, the present invention can be seen to provide a
first embodiment of a lower cost high strength nickel based alloy that broadly comprises
from 3.0 to 5.2 wt% chromium, from 1.5 to 3.0 wt% molybdenum, from 6.0 to 12.5 wt%
tungsten, from 5.0 to 11 wt% tantalum, from 5.5 to 6.5 wt% aluminum, from 11 to 14
wt% cobalt, from 0.001 to 1.75 wt% rhenium, from 0.2 to 0.6 wt% hafnium, up to 0.05
wt% yttrium, up to 3.0 wt% ruthenium, and the balance nickel.
[0007] From a second aspect, the present invention can be seen to provide another embodiment
of a lower cost high strength nickel based alloy broadly comprises from 1.0 to 3.0
wt% chromium, up to 2.5 wt% molybdenum, from 11 to 16 wt% tungsten, from 4.0 to 8.0
tantalum, from 5.7 to 6.5 wt% aluminum, from 11 to 15 wt% cobalt, from 2.0 to 4.0
wt% rhenium, from 0.2 to 0.6 wt% hafnium, up to 0.05 wt% yttrium, up to 3.0 wt% ruthenium,
and the balance nickel.
[0008] Certain preferred embodiments of the lower cost high strength nickel based superalloys
of the present invention will now be described in greater detail and by way of example
only and with reference to the accompanying drawings, in which:
FIG. 1 is a plot of tantalum weight % vs. tungsten weight %; and
FIG. 2 is a bubble chart of Ta weight% vs. tungsten weight% with the bubble size proportional
to (Re + Ru) weight %.
[0009] The combinations of compositions with the elements Ti, Nb, Ta, Mo, W, Re, and Ru
along with primary elements Ni, Co, Cr, and Al, is so large that it is cost prohibitive
to explore the entire alloy space. Traditionally, alloys are evolved based on prior
experience and once the target performance benefit is realized, there is little motivation
to visit the unexplored alloy compositional space. There is no simple quantitative
way to map out a space bounded by a dozen elements and pinpoint the gaps. In a limited
sense, a bubble plot of Ta weight % vs. W weight %, as shown in Figure 1, graphically
represents maps out a desirable space. In this plot, the size of the bubble or plotting
point for each alloy is proportional to the total concentration of (Re + Ru) in the
alloys of interest.
[0010] Prior to the development of the first generation single crystal alloy PWA 1480, the
best known equiaxed and columnar grain alloys were based on Mar M200, which contain
12.5 weight% of W. Also the alloy contained 2.0 weight % Ti. Development of PWA 1480
was marked by the addition of 12 weight% Ta. Subsequent development of second generation
single crystal alloys such as PWA 1484 all had a marked absence of Ti. An improved
second generation DS alloy, PWA 1426, was developed with Re additions similar to PWA
1484. The fourth generation of single crystal alloys such as PWA 1497 have an increase
in Re concentration concurrent with Ru additions. As can be seen in Fig. 1, these
alloys do not overlap in the Ta, W, (Re + Ru) space. In these higher strength alloys,
the concentration of Ta never decreased below 4 wt% and W never increased beyond 6.0
wt%.
[0011] The successful development of second generation single crystal alloys has been attributed
to Re additions and it is generally believed that Re makes the lattice misfit between
the γ' precipitate and the γ-matrix become more negative. Re is also thought to reduce
the coarsening rate of the γ' phase, contributing to improving creep strength.
[0012] Useful alloys are listed in Table I and are also depicted in FIGS. 1 and 2. Fig.
1 clearly depicts that in Ta weight % vs. W weight % plots, current production alloys
are outside the alloy space. The Ta in production alloys is showed by the diamond
points 10 on FIG. 1 and the space with the Ta in the alloys set forth herein are shown
by the squares in the space 12. The same information is plotted in FIG. 2 as a bubble
chart, where the size of plotting points is proportional to the concentration of (Re
+ Ru). In FIG. 2, bubble 20 is alloy PWA 1422, bubble 22 is alloy PWA 1480, bubble
24 is alloy PWA 1497, bubble 26 is alloy PWA 1484, bubble 28 is alloy 2a in Table
I, bubble 30 is alloy 2b in Table I, bubble 32 is alloy 1a in Table I, bubble 34 is
alloy 1b in Table I, bubble 36 is alloy 3a in Table I, bubble 38 is alloy 3b in Table
I, bubble 40 is alloy 3c in Table I, bubble 42 is alloy PWA 1426, bubble 44 is alloy
PWA 1426a, and bubble 46 is alloy PWA 1426b.
TABLE I
Alloy |
Cr |
Mo |
W |
Ta |
Al |
Co |
Re |
Ru |
Hf |
P |
Density |
Creep Life |
Nv3B |
Stability |
COMMENTS |
Single Crystal |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
1a |
4 |
2 |
11 |
6 |
6 |
12.5 |
0 |
0 |
|
48.5 |
0.322 |
PWA 1484 |
2.07 |
S |
Creep = 1484 No Re/Ru |
1b |
5 |
2 |
9 |
6 |
6 |
12.5 |
0 |
3 |
|
48.5 |
0.318 |
PWA 1484 |
2.07 |
S |
Creep 1484 No Re (3Ru) |
1c |
4 |
2 |
9 |
6 |
6 |
12.5 |
1.5 |
0 |
|
48.5 |
0.32 |
PWA 1484 |
2.04 |
S |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
2a |
2 |
1.75 |
11.5 |
6 |
6 |
12.5 |
3 |
3 |
|
58 |
0.331 |
PWA 1497 |
2.02 |
S |
Creep = 1497 with 3Re, 3Ru |
2b |
2 |
1 |
12.5 |
6 |
6 |
12.5 |
3 |
0 |
|
55.75 |
0.331 |
1497-15F |
2.02 |
S |
Creep - 1497 with 3Re, 0Ru |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
3a |
2 |
1.75 |
15.5 |
6 |
6 |
12.5 |
0 |
3 |
|
58 |
0.334 |
PWA 1497 |
2.09 |
S |
Creep = 1497 with ORe, 3Ru |
3b |
2 |
2 |
13.5 |
6 |
6 |
12.5 |
1.5 |
0 |
|
55.25 |
0.331 |
1497 -20F |
2.08 |
S |
creep < 1497 with 1.5Re, ORu |
3c |
2 |
2 |
15 |
6 |
6 |
12.5 |
0 |
0 |
|
54.5 |
0.331 |
1497-25F |
2.08 |
S |
creep <1497 with ORe, ORu |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
PWA 1484 |
5 |
1.9 |
5.9 |
8.7 |
5.65 |
10 |
3 |
0 |
|
48 |
0.323 |
|
2.08 |
|
|
PWA 1497 |
2 |
1.8 |
6 |
8.25 |
5.65 |
16.5 |
6 |
3 |
|
58 |
0.331 |
|
|
|
|
DS |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
PWA 1426 |
6.4 |
1.7 |
6.4 |
4 |
5.9 |
12.5 |
3 |
0 |
1.5 |
44.9 |
0.316 |
Base |
2.07 |
S |
|
PWA 1426a |
6.4 |
1.7 |
8.4 |
4 |
5.9 |
12.5 |
1.5 |
0 |
1.5 |
44.9 |
0.318 |
Base |
2.11 |
S |
creep = 1426 1.5Re |
PWA 1426b |
6.4 |
1.7 |
10.4 |
4 |
5.9 |
12.5 |
0 |
0 |
1.5 |
44.9 |
0.322 |
Base |
2.24 |
Mg |
creep=14260Re |
[0013] Listed in Table I are baseline compositions of the second and fourth generation single
crystal alloys PWA 1484 and PWA 1497, respectively, and the second generation columnar
grain (DS) alloy PWA 1426. It can be seen from FIG. 2 that using the useful alloys
described herein, one can achieve the same level of creep resistance as PWA 1426,
for reducing Re-containing alloys (PWA 1426a and PWA 1426b), by increasing the W content
of these alloys.
[0014] One embodiment of a useful alloy contains from 3.0 to 5.2 wt% chromium, from 1.5
to 3.0 wt% molybdenum, from 6.0 to 12.5 wt% tungsten, from 5.0 to 11 wt% tantalum,
from 5.5 to 6.5 wt% aluminum, from 11 to 14 wt% cobalt, from 0.001 to 1.75 wt% rhenium,
from 0.2 to 0.6 wt% hafnium, up to 0.05 wt% yttrium, and the balance nickel.
[0015] Table II is a comparison of alloys having compositions within the aforesaid range
with Rene N5. The data shows the alloys described herein to have higher density, an
equivalent or better life, better yield strength, and equivalent or better ultimate
tensile strength than Rene N5.
TABLE II
|
Casting Chemistry Weight % |
|
|
Act lbs/cu in |
1850F/38ksi |
1200F Tensile |
|
Cr |
Mo |
W |
Ta |
Al |
Co |
Re |
Hf |
Density |
Life |
1% |
EI |
YS |
UTS |
EI |
Alloy 1 |
3.97 |
2.07 |
10.82 |
6.07 |
6.15 |
12.81 |
0 |
0.32 |
0.320 |
40.2 |
16 |
38.1 |
124.5 |
140.2 |
22 |
|
|
|
|
|
|
|
|
|
|
31.7 |
10 |
23.4 |
124.8 |
139.1 |
23.1 |
|
|
|
|
|
|
|
|
|
|
37.5 |
16 |
25.6 |
126.2 |
139.3 |
24.2 |
|
|
|
|
|
|
|
|
|
AVE |
36.5 |
14 |
29 |
125.2 |
139.5 |
23.1 |
Alloy 2 |
3.99 |
2.03 |
8.81 |
6.01 |
5.78 |
12.23 |
1.54 |
0.34 |
0.320 |
61.7 |
24 |
28.4 |
135.8 |
143.5 |
21.8 |
|
|
|
|
|
|
|
|
|
|
63.1 |
24 |
39.3 |
130.1 |
137.9 |
19 |
|
|
|
|
|
|
|
|
|
|
68.6 |
26 |
36.9 |
130.7 |
139.1 |
21.8 |
|
|
|
|
|
|
|
|
|
AVE |
64.5 |
24.7 |
34.9 |
132.2 |
140.2 |
20.9 |
Alloy 3 |
5.09 |
2.09 |
10.97 |
5.62 |
6.15 |
12.9 |
0 |
0.36 |
0.319 |
48.7 |
16 |
41.3 |
120.6 |
139 |
17.8 |
|
|
|
|
|
|
|
|
|
|
45.5 |
14 |
38.3 |
127.3 |
145.4 |
17.2 |
|
|
|
|
|
|
|
|
|
|
40.6 |
13 |
37 |
127.6 |
147.2 |
21.1 |
|
|
|
|
|
|
|
|
|
AVE |
44.9 |
14.3 |
38.9 |
125.2 |
143.9 |
18.7 |
Alloy 4 |
5.01 |
2.08 |
9.41 |
7.04 |
5.9 |
12.45 |
0 |
0.35 |
0.320 |
41.2 |
14 |
36 |
130.2 |
145 |
21.9 |
|
|
|
|
|
|
|
|
|
|
41.1 |
14 |
37.2 |
134 |
150 |
21.3 |
|
|
|
|
|
|
|
|
|
|
42.8 |
14 |
41.7 |
133.3 |
146.3 |
20.9 |
|
|
|
|
|
|
|
|
|
AVE |
41.7 |
14 |
38.3 |
132.5 |
147.1 |
21.4 |
Alloy 5 |
3.93 |
2.06 |
8.87 |
9.03 |
5.89 |
12.38 |
0 |
0.34 |
0.323 |
39.6 |
10 |
40.1 |
132.2 |
144.7 |
13.5 |
|
|
|
|
|
|
|
|
|
|
38.6 |
9 |
35.9 |
137.7 |
149.6 |
25.6 |
|
|
|
|
|
|
|
|
|
|
43.4 |
13 |
37.4 |
134.9 |
146.9 |
22 |
|
|
|
|
|
|
|
|
|
AVE |
40.5 |
10.7 |
37.8 |
134.9 |
147.1 |
20.4 |
Alloy 6 |
5.04 |
2.1 |
11.82 |
5.65 |
5.58 |
12.46 |
0 |
0.34 |
0.323 |
40.1 |
17 |
29.9 |
138.1 |
152.7 |
18.9 |
|
|
|
|
|
|
|
|
|
|
40.1 |
14 |
26.1 |
140.8 |
154.1 |
23.2 |
|
|
|
|
|
|
|
|
|
|
39.6 |
15 |
24 |
139.5 |
154.9 |
23.2 |
|
|
|
|
|
|
|
|
|
AVE |
39.9 |
15.3 |
26.7 |
139.5 |
153.4 |
21.8 |
Alloy 7 |
4.51 |
2.06 |
7.08 |
10.07 |
5.8 |
12.84 |
1.43 |
0.33 |
0.3235 |
66.6 |
26 |
42.3 |
148 |
179.6 |
9.3 |
|
|
|
|
|
|
|
|
|
|
65.2 |
25 |
39.4 |
148.2 |
179.2 |
12.6 |
|
|
|
|
|
|
|
|
|
|
59.9 |
20 |
36 |
149.6 |
181 |
7.8 |
|
|
|
|
|
|
|
|
|
AVE |
63.9 |
23.7 |
39.2 |
148.6 |
179.9 |
9.9 |
Alloy 8 |
5.08 |
2.05 |
8.81 |
7.32 |
6.14 |
12.85 |
0 |
0.34 |
0.317 |
35.8 |
11 |
41.7 |
129.8 |
148.3 |
15.8 |
|
|
|
|
|
|
|
|
|
|
37.2 |
12 |
40 |
129.4 |
148 |
16.8 |
|
|
|
|
|
|
|
|
|
|
39.4 |
14 |
41.8 |
128.2 |
145.4 |
18.4 |
|
|
|
|
|
|
|
|
|
AVE |
37.5 |
12.3 |
41.2 |
129.1 |
147.2 |
17 |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Rene N5 Nom |
7 |
1.5 |
5 |
6.5 |
6.2 |
7.5 |
3 |
0.15 |
0.312 |
40.5 |
|
|
122 |
145 |
|
[0016] A second embodiment of a useful alloy contains from 4.0 to 5.0 wt% chromium, from
1.7 to 2.3 wt% molybdenum, from 7.0 to 12.5 wt% tungsten, from 5.5 to 10 wt% tantalum,
from 5.6 to 6.25 wt% aluminum, from 11.5 to 13.5 wt% cobalt, from 0.001 to 1.75 wt%
rhenium, from 0.2 to 0.4 wt% hafnium, from 0.001 to 0.01 wt% yttrium, and the balance
nickel.
[0017] A third embodiment of a useful alloy contains from 1.0 to 3.0 wt% chromium, up to
2.5 wt% molybdenum, from 11 to 16 wt% tungsten, from 4.0 to 8.0 tantalum, from 5.7
to 6.5 wt% aluminum, from 11 to 15 wt% cobalt, from 2.0 to 4.0 wt% rhenium, from 0.2
to 0.6 wt% hafnium, up to 0.05 wt% yttrium and the balance nickel.
[0018] A fourth embodiment of a useful alloy contains from 1.5 to 2.5 wt% chromium, from
0.5 to 1.5 wt% molybdenum, from 11.5 to 13.5 wt% tungsten, from 5.0 to 7.0 tantalum,
from 5.8 to 6.25 wt% aluminum, from 11.5 to 13.5 wt% cobalt, from 2.5 to 3.5 wt% rhenium,
from 0.2 to 0.4 wt% hafnium, from 0.001 to 0.01 wt% yttrium, and the balance nickel.
[0019] The above alloys may contain up to 3.0 wt% ruthenium. The total rhenium and ruthenium
content of each of the alloys may be no greater than 6.0 wt%.
[0020] Oxidation resistance can be maintained by the addition of at least 15 - 30 ppm yttrium
or other equivalent active elements such as Ca, Mg, and other rare earth elements.
Previously, yttrium and other rare earth additions have not been added to alloys containing
elevated levels of W, i.e. greater than 6.0 weight%.
[0021] The alloys described herein can fulfill the low cost requirements. Since Re and Ru
raw material prices have risen in the last few years, reducing their concentration
in new alloys by 50% or more (compared to existing second generation and higher alloys)
will have a significant effect on master heat cost.
[0022] It should be apparent that there has been provided in accordance with the present
disclosure lower cost high strength single crystal superalloys with reduced rhenium
and ruthenium content. While the superalloys have been described in the context of
specific embodiments thereof, other unforeseeable alternatives, variations and modifications
make become apparent to those skilled in the art having read the foregoing description.
Accordingly, it is intended to embrace those alternatives, modifications, and variations
as fall within the broad scope of the appended claims.
1. A nickel based alloy consisting essentially of from 3.0 to 5.2 wt% chromium, from
1.5 to 3.0 wt% molybdenum, from 6.0 to 12.5 wt% tungsten, from 5.0 to 11 wt% tantalum,
from 5.5 to 6.5 wt% aluminum, from 11 to 14 wt% cobalt, up to 1.75 wt% rhenium, from
0.2 to 0.6 wt% hafnium, up to 0.05 wt% yttrium, up to 3.0 wt% ruthenium, and the balance
nickel.
2. The nickel based alloy of claim 1, wherein said chromium is present in an amount from
4.0 to 5.0 wt%.
3. The nickel based alloy of claim 1 or 2, wherein said molybdenum is present in an amount
from 1.7 to 2.3 wt%.
4. The nickel based alloy of claim 1, 2 or 3, wherein said tungsten is present in an
amount from 7.0 to 12 wt%.
5. The nickel based alloy of any preceding claim, wherein said tantalum is present in
an amount from 5.5 to 10 wt%.
6. The nickel based alloy of any preceding claim, wherein said aluminum is present in
an amount from 5.6 to 6.25 wt%.
7. The nickel based alloy of any preceding claim, wherein said cobalt is present in an
amount from 11.5 to 13.5 wt%.
8. The nickel based alloy of any preceding claim, wherein said rhenium is present in
an amount from 0.001 to 1.75 wt%, said hafnium is present in an amount from 0.2 to
0.4 wt%, and said yttrium is present in an amount from 0.001 to 0.01 wt%.
9. The nickel based alloy of any preceding claim, wherein the total ruthenium and rhenium
content is no greater than 6.0 wt%.
10. A nickel based alloy consisting essentially of from 1.0 to 3.0 wt% chromium, up to
2.5 wt% molybdenum, from 11 to 16 wt% tungsten, from 4.0 to 8.0 tantalum, from 5.7
to 6.5 wt% aluminum, from 11 to 15 wt% cobalt, from 2.0 to 4.0 wt% rhenium, from 0.2
to 0.6 wt% hafnium, up to 0.05 wt% yttrium, up to 3.0 wt% ruthenium, and the balance
nickel.
11. The nickel based alloy of claim 10, wherein said chromium is present in an amount
from 1.5 to 2.5 wt%, said molybdenum is present in an amount from 0.5 to 1.5 wt%.
12. The nickel based alloy of claim 10 or 11, wherein said tungsten is present in an amount
from 11.5 to 13.5 wt%.
13. The nickel based alloy of claim 10, 11 or 12, wherein said tantalum is present in
an amount from 5.0 to 7.0 wt%, said aluminum is present in an amount from 5.8 to 6.25
wt%, and said cobalt is present in an amount from 11.5 to 13.5 wt%.
14. The nickel based alloy of any of claims 10 to 13, wherein said rhenium is present
in amount from 2.5 to 3.5 wt%, said hafnium is present in an amount from 0.2 to 0.4
wt%, and said yttrium is present in an amount of from 0.001 to 0.01 wt%.
15. The nickel based alloy of any of claims 10 to 14, wherein the total ruthenium and
rhenium content is no greater than 6.0 wt%.