US20130142637A1

US20130142637A1 - Low rhenium single crystal superalloy for turbine blades and vane applications

Info

Publication number: US20130142637A1
Application number: US13/311,626
Authority: US
Inventors: Kenneth Harris; Jacqueline B. Wahl
Original assignee: Cannon Muskegon Corp
Current assignee: Cannon Muskegon Corp
Priority date: 2011-12-06
Filing date: 2011-12-06
Publication date: 2013-06-06
Also published as: US20180100401A1; IL219180A; ES2562011T3; US10519787B2; IL219180A0; KR101470069B1; EP2612935B1; JP2013119668A; JP5746998B2; EP2612935A3; CA2774730A1; KR20130063445A; EP2612935A2; CA2774730C

Abstract

A low rhenium nickel-base superalloy for single crystal casting that exhibits excellent high temperature creep resistance, while also exhibiting other desirable properties for such alloys, comprises 5.60% to 5.80% aluminum by weight, 9.4% to 9.9% cobalt by weight, 4.9% to 5.5% chromium by weight, 0.08% to 0.35% hafnium by weight, 0.50% to 0.70% molybdenum by weight, 1.4% to 1.6% rhenium by weight, 8.1% to 8.5% tantalum by weight, 0.60% to 0.80 titanium by weight, 7.6 to 8.0% tungsten by weight the balance comprising nickel and minor amounts of incidental impurity elements.

Description

FIELD

Disclosed are single crystal nickel-base superalloys exhibiting excellent high temperature creep resistance, while having a reduced or low rhenium content, without deleteriously affecting other relevant characteristics for many turbine engine airfoil applications.

BACKGROUND

Because of a worldwide growing demand for products that have customarily required substantial quantities of relatively scarce metal elements, both the demand and prices of rare metal elements have sharply increased. As a result, manufacturers are searching for new technologies that will reduce or eliminate the need for these metal elements.
Rhenium is an example of a truly rare metal that is important to various industries. It is recovered in very small quantities as a by-product of copper-molybdenum and copper production. In addition to its high cost, use of rhenium presents a supply chain risk of both economic and strategic consequence.
Rhenium has been widely employed in the production of nickel-base superalloys used to cast single crystal gas turbine components for jet aircraft and power generation equipment. More specifically, rhenium is used as an additive in advanced single crystal superalloys for turbine blades, vanes and seal segments, because of its potent effect at slowing diffusion and thus slowing creep deformation, particularly at high temperatures (e.g., in excess of 1,000 degrees C.) for sustained periods of time. High temperature creep resistance is directly related to the useful service life of gas turbine components and turbine engine performance such as power output, fuel burn and carbon dioxide emissions.
Typical nickel-base superalloys used for single crystal castings contain from about 3% rhenium to about 7% rhenium by weight. Although rhenium has been used as only a relatively minor additive, it has been regarded as critical to single crystal nickel-base superalloys to inhibit diffusion and improve high temperature creep resistance, it adds considerably to the total cost of these alloys.
From the foregoing discussion, it should be apparent that it would be extremely desirable to develop single crystal nickel-base superalloys that exhibit excellent high temperature creep resistance, while significantly reducing the need for rhenium alloying additions, and while retaining other desirable properties such as creep-rupture, low cycle fatigue (LCF) strength and oxidation coating performance.

SUMMARY

The low rhenium single crystal nickel-base superalloys disclosed herein rely on, among other things, balancing the refractory metal elements (tantalum, tungsten, rhenium and molybdenum) at a total amount of from about 18% to 19% by weight in order to achieve good creep-rupture mechanical properties along with acceptable alloy phase stability, including freedom from excessive deleterious topological close-packed (TCP) phases that are rich in tungsten, rhenium and chromium, while substantially reducing the rhenium content.
It has been discovered that a low rhenium single crystal nickel-base superalloy exhibiting excellent high temperature creep resistance and other properties well suited for use in casting gas turbine components can be achieved in an alloy composition containing 5.60% to 5.80% aluminum by weight, 9.4% to 9.9% cobalt by weight, 4.9% to 5.5% chromium by weight, 0.08% to 0.35% hafnium by weight, 0.50% to 0.70% molybdenum by weight, 1.4% to 1.6% rhenium by weight, 8.1% to 8.5% tantalum by weight, 0.60% to 0.80% titanium by weight, 7.6% to 8.0% tungsten by weight, and the balance comprising nickel and minor amounts of incidental elements, the total amount of incidental elements being less than 1% by weight.
In the case of certain embodiments of the invention, the incidental elements of the nickel-base superalloy are present at maximum amounts of 100 ppm carbon, 0.04% silicon, 0.01% manganese, 3 ppm sulfur, 30 ppm phosphorous, 30 ppm boron, 0.10% niobium, 150 ppm zirconium, 0.01% copper, 0.15% iron, 0.10% vanadium, 0.10% ruthenium, 0.15% platinum, 0.15% palladium, 200 ppm magnesium, 5 ppm nitrogen (generally in the form of a metal nitride or carbonitride), 5 ppm oxygen (generally in the form of a stable metal oxide), and other trace elements present in amounts of about 25 ppm or less.
In accordance with certain embodiments, the trace elements of the incidental elements in the nickel-base superalloys are present at maximum amounts of 2 ppm silver, 0.2 ppm bismuth, 10 ppm gallium, 25 ppm calcium, 1 ppm lead, 0.5 ppm selenium, 0.2 ppm tellurium, 0.2 ppm thallium, 10 ppm tin, 2 ppm antimony, 2 ppm arsenic, 5 ppm zinc, 2 ppm mercury, 2 ppm cadmium, 2 ppm germanium, 2 ppm gold, 2 ppm indium, 20 ppm sodium, 10 ppm potassium, 20 ppm barium, 30 ppm phosphorous, 2 ppm uranium, and 2 ppm thorium.
In certain embodiments in which enhanced oxidation resistance and/or enhanced thermal barrier coating life are desired, sulfur is present at a maximum amount of 0.5 ppm, and lanthanum and yttrium are added to target an amount of total lanthanum and yttrium of from about 5 ppm to about 80 ppm in the single crystal components cast from the alloy.
In accordance with certain embodiments for large industrial gas turbine (IGT) single crystal applications in which a low angle boundary (LAB) strengthening of up to 12 degrees is desired, carbon is added in an amount from about 0.02% to about 0.05%, and boron is added in an amount of from about 40 ppm to about 100 ppm.
In accordance with certain embodiments, the alloy has a density that is about 8.90 gms/cc or less, such as about 8.85 gms/cc (kg/dm³) at room temperature.

BRIEF DESCRIPTION OF THE DRAWINGS

FIGS. 1A, 1B and 1C are optical micrographs of castings made from the disclosed alloys (LA-11825, CMSX®-8, test bar #N926, solutioned+2050° F./4 hours, gage area).

FIGS. 2A, 2B and 2C are scanning electron micrographs of castings made using the disclosed alloys (LA-11825, CMSX®-8, test bar #N926, solutioned+2050° F./4 hours, gage area).

FIGS. 3 and 4 are Larson-Miller stress-rupture and stress-1.0% creep diagrams showing that the alloys disclosed herein have properties similar to advanced CMSX-4® single crystal nickel-base superalloy having a substantially higher rhenium content, up to 1900° F. (1040° C.).

FIGS. 5A, 5B and 5C are optical micrographs demonstrating that the post-test phase stability of single crystal test bar castings made using the disclosed alloys is surprisingly good, and that there are no detectable TCP phases (LA-11848, CMSX®-8, test bar #A925, 1562° F./94.4 ksi/211.9 hours, fracture area).

FIGS. 6A, 6B and 6C are scanning electron micrographs demonstrating that the post-test phase stability of single crystal test bar castings made using the disclosed alloys is surprisingly good, and that there are no detectable TCP phases (LA-11848, CMSX®-8, test bar #A925, 1562° F./94.4 ksi/211.9 hours, fracture area).

FIGS. 7A, 7B and 7C are optical micrographs demonstrating that the post-test phase stability of single crystal test bar castings made using the disclosed alloys is surprisingly good, and that there are no detectable TCP phases (LA-11848, CMSX®-8, test bar #A925, 1562° F./94.4 ksi/211.9 hours, gage area).

FIGS. 8A, 8B and 8C are scanning electron micrographs demonstrating that the post-test phase stability of single crystal test bar castings made using the disclosed alloys is surprisingly good, and that there are no detectable TCP phases (LA-11848, CMSX®-8, test bar #A925, 1562° F./94.4 ksi/211.9 hours, gage area).

FIGS. 9A, 9B and 9C are optical micrographs demonstrating that the post-test phase stability of single crystal test bar castings made using the disclosed alloys is surprisingly good, and that there are no detectable TCP phases (LA-11848, CMSX®-8, test bar #E926, 1800° F./36 ksi/246.7 hours, fracture area).

FIGS. 10A, 10B and 10C are scanning electron micrographs demonstrating that the post-test phase stability of single crystal test bar castings made using the disclosed alloys is surprisingly good, and that there are no detectable TCP phases (LA-11848, CMSX®-8, test bar #E926, 1800° F./36 ksi/246.7 hours, fracture area).

FIGS. 11A, 11B and 11C are optical micrographs demonstrating that the post-test phase stability of single crystal test bar castings made using the disclosed alloys is surprisingly good, and that there are no detectable TCP phases (LA-11848, CMSX®-8, test bar #E926, 1800° F./36 ksi/246.7 hours, gage area).

FIGS. 12A, 12B and 12C are scanning electron micrographs demonstrating that the post-test phase stability of single crystal test bar castings made using the disclosed alloys is surprisingly good, and that there are no detectable TCP phases (LA-11848, CMSX®-8, test bar #E926, 1800° F./36 ksi/246.7 hours, gage area).

FIGS. 13A, 13B and 13C are optical micrographs demonstrating that the post-test phase stability of single crystal test bar castings made using the disclosed alloys is surprisingly good, and that there are no detectable TCP phases (LA-11848, CMSX®-8, test bar #L926, 2050° F./15 ksi/285.4 hours, fracture area).

FIGS. 14A, 14B and 14C are scanning electron micrographs demonstrating that the post-test phase stability of single crystal test bar castings made using the disclosed alloys is surprisingly good, and that there are no detectable TCP phases (LA-11848, CMSX®-8, test bar #L926, 2050° F./15 ksi/285.4 hours, fracture area).

FIGS. 15A, 15B and 15C are optical micrographs demonstrating that the post-test phase stability of single crystal test bar castings made using the disclosed alloys is surprisingly good, and that there are no detectable TCP phases (LA-11848, CMSX®-8, test bar #L926, 2050° F./15 ksi/285.4 hours, gage area).

FIGS. 16A, 16B and 16C are scanning electron micrographs demonstrating that the post-test phase stability of single crystal test bar castings made using the disclosed alloys is surprisingly good, and that there are no detectable TCP phases (LA-11848, CMSX®-8, test bar #L926, 2050° F./15 ksi/285.4 hours, gage area).

FIGS. 17A, 17B and 17C are optical micrographs showing adequate solutioning and/or homogenizing of an alloy casting using a shortened heat treatment cycle (LA-11862, CMSX®-8, test bar #A926, solutioned to 2408° F./8 hours, longitudinal).

FIG. 18 is a Larson-Miller stress-rupture graphs showing the surprisingly good stress-rupture life properties of single crystal test bars and turbine blade castings made from the disclosed alloys.

FIGS. 19A, 19B and 19C are optical micrographs demonstrating that the post-test phase stability of single crystal test bar castings made using the disclosed alloys is surprisingly good, and that there are no detectable TCP phases (LA-11890, CMSX®-8, test bar #A926, 2050° F./15 ksi (1121° C./103 MPa)/271.8 hours, gage area).

FIGS. 20A, 20B and 20C are scanning electron micrographs demonstrating that the post-test phase stability of single crystal test bar castings made using the disclosed alloys is surprisingly good, and that there are no detectable TCP phases (LA-11890, CMSX®-8, test bar #A926, 2050° F./15 ksi (1121° C./103 MPa)/271.8 hours, gage area).

FIG. 21 is a drawing in cross section of a single crystal solid turbine blade cast from an alloy as disclosed herein which has the facility to machine both mini-bar and mini-flat specimens for machined-from-blade (MFB) stress-rupture testing.

FIGS. 22A, 22B and 22C are optical micrographs demonstrating that the post-test phase stability of single crystal test bar castings made using the disclosed alloys is surprisingly good, and that there are negligible detectable TCP phases (needles) (LA-11895, CMSX®-8, test bar #R926, 2000° F. (1093° C./83 MPa)/12 ksi/1979.9 hours, gage area).

FIGS. 23A, 23B and 23C are scanning electron micrographs demonstrating that the post-test phase stability of single crystal test bar castings made using the disclosed alloys is surprisingly good, and that there are negligible detectable TCP phases (needles) (LA-11895, CMSX®-8, test bar #R926, 2000° F. (1093° C./83 MPa)/12 ksi/1979.9 hours, gage area).

DETAILED DESCRIPTION

The low-rhenium nickel-base superalloys for single crystal casting disclosed herein will be designated “CMSX®-8” alloys, and will be referred to as such herein. The term “CMSX” is a trademark registered to Cannon-Muskegon Corporation for use in connection with the sale of a family of single crystal (SX) nickel-base superalloys.
Unless otherwise indicated herein, all amounts of elements are given as a percentage by weight or in parts per million (ppm) by weight based on the entire weight of the alloy composition.
Single crystal superalloys and castings have been developed to exhibit an array of outstanding properties including high temperature creep resistance, long fatigue life, oxidation and corrosion resistance, and solid solution strengthening, with desired casting properties with low rejection rates, and phase stability, among others. While it is possible to optimize a single additive for a particular property, the effects on other properties are often extremely unpredictable. Generally, the relationships among the various properties and various elemental components are extremely complex and unpredictable such that it is surprising when a substantial change can be made to the composition without deleteriously affecting at least certain essential properties.
With the embodiments disclosed herein, refractory metal elements (tantalum, tungsten, rhenium and molybdenum) (Table 1) were maintained at a total amount of from about 18% to about 19% by weight, while balancing the amounts of the refractory elements to achieve good creep-rupture mechanical properties along with acceptable alloy phase stability (freedom from excessive deleterious topological close-packed (TCP) phases—normally tungsten, rhenium and chromium rich in this type of alloy). Chromium and cobalt amounts are targeted accordingly to ensure this required phase stability. The high tantalum at approximately 8% is designed to give good single crystal castability and freedom from “freckling” defects, and, along with the 5.7% aluminum and the 0.7% titanium, appropriate γ′ volume fraction at approximately 70% and low negative γ/γ′ mismatch for high temperature creep strength, and acceptable room temperature density of about 8.85 gms/cc (kg/dm³). The density of CMSX-4® is 8.70 gms/cc (kg/dm³) and PWA 1484 is 8.95 gms/cc (kg/dm³). Aluminum, tantalum and titanium are targeted at γ′ volume fraction (Vf) attainment, along with low molybdenum for good high temperature oxidation properties. The small hafnium addition is required for coating life attainment at high temperatures.
Typical chemistry for the alloys disclosed and claimed herein are listed in Table 1. However, there are certain minor variations. First, in order to achieve enhanced oxidation resistance and/or enhanced thermal barrier coating life, it is desirable to add lanthanum and/or yttrium in amounts such that the total of lanthanum and yttrium is targeted to provide from about 5 to 80 ppm in the single crystal castings made from the alloys. As another variation, in the case of large industrial gas turbine (IGT) single crystal applications where low angle boundary (LAB) strengthening is provided up to 12 degrees, carbon and boron additions are targeted in the range from about 0.02% to 0.05% and 40-100 ppm, respectively.

TABLE 1

CHEMISTRY (WT %/ppm) SPECIFICATIONS CMSX ®-8 ALLOY
Aero engine Applications

C

	100	ppm	Ta	8.1-8.5
Si	.04%	Max	Ti	.60-.80
Mn	.01%	Max	W	7.6-8.0

S

3

ppm Max

Zr

150

ppm Max

Al

5.60-5.85

Cu

.01%

Max

B

	30	ppm Max	Fe	.15%	Max
Cb (Nb)	.10%	Max	V	.10%	Max

Co	9.4-9.9	Ru	.10%	Max
Cr	4.9-5.5	Pt	.15%	Max
Hf	.08-.35	Pd	.15%	Max
Mo	.50-.70	Mg	200	ppm Max
Ni	Balance	[N]	5	ppm Max
Re	1.4-1.6	[O]	5	ppm Max

Enhanced oxidation resistance/coating and

thermal barrier coating (TBC) life

	S	0.5	ppm max
	La + Y	5-80	ppm (In the SX castings).

Industrial Gas Turbine (IGT) SX Applications

Low angle boundary (LAB) Strengthened up to 12°.

C	0.05%	Max
B
100	ppm Max

TRACE ELEMENT CONTROLS - ALL APPLICATIONS

Ag	2	ppm Max	Hg	2	ppm Max
Bi	.2	ppm Max	Cd	2	ppm Max
Ga
10	ppm Max	Ge	2	ppm Max
Ca	25	ppm Max	Au	2	ppm Max
Pb
1	ppm Max	In	2	ppm Max
Se	.5	ppm Max	Na		20	ppm Max
Te	.2	ppm Max	K		10	ppm Max
Tl	.2	ppm Max	Ba		10	ppm Max
Sn
10	ppm Max	P		30	ppm Max
Sb	2	ppm Max	U	2	ppm Max
As	2	ppm Max	Th	2	ppm Max
Zn
5	ppm Max

Density: 8.85 gms/cc (kg/dm³).

The invention will be described below with respect to certain illustrative, non-limiting embodiments that will facilitate a better understanding.
A 470 lb 100% virgin initial heat of CMSX®-8 alloy was melted in May 2011 in the CM V-5 Consarc VIM furnace using aim chemistry to CM KH May 20, 2011 (CM CRMP #81-1708 Issue 1). The heat (5V0460) chemistry is shown in Table 2.
Two molds (#s 925 and 926) of SX NNS DL-10 test bars were cast to CMSX-4® casting parameters by Rolls-Royce Corporation (SCFO). DL-10 test bar yield at 23 fully acceptable out of a total 24 cast was excellent.
These DL-10 test bars were solutioned/homogenized and double aged heat treated at Cannon-Muskegon Corporation as follows—based on prior work with a precursor similar family alloy designated CMSX®-7.
Solutioning and Homogenization

- 2 hrs/2340° F. (1282° C.)+2 hrs/2360° F. (1293° C.)
- +4 hrs/2380° F. (1304° C.)+4 hrs/2390° F. (1310° C.)
- +12 hrs/2400° F. (1316° C.) AC (air cool)—ramping up at 1° F./min. between steps
  - +
- Double Aged Heat Treatment
- 4 hrs/2050° F. (1121° C.) AC+20 hrs/1600° F. (871° C.) AC

Good microstructure attainment is evident in FIGS. 1-2—complete γ′ solutioning, little remnant γ/γ′ eutectic, no incipient melting and approximately 0.45 μm average cubic, aligned γ′, indicating appropriate γ/γ′ mismatch and γ/γ′ inter-facial chemistry, following the 4 hr/2050° F. (1121° C.) high temperature age.
Creep- and stress-rupture specimens were low stress ground and tested by Joliet Metallurgical Labs, with the results to date shown in Table 3. Larson-Miller stress-rupture and stress-1.0% creep (FIGS. 3 & 4) show CMSX®-8 has similar and surprisingly good creep strength/stress-rupture life properties to CMSX-4® alloy (3% Re) up to approximate 1850° F.-1900° F. (1010-1038° C.), with fall-off at 2050° F. (1121° C.) due to its cost saving lower Re (1.5%) content. All these properties are significantly higher than Rene' N-5 (3% Re) and Rene' N-515 (low Re) alloys (JOM, Volume 62, Issue 1, pp. 55-57).

TABLE 2

HEAT #5V0460 CMSX ®-8 - 100%
VIRGIN CHEMISTRY (WT ppm/%)

C

9

ppm

Cu

<.001

	Si	<.02	Fe	.010
	Mn	<.001	V	<.005

S

1

ppm

Ru

<.01

Al

5.72

Pt

<.001

B

<20

ppm

Pd

<.001

Cb (Nb)	<.05	Mg	<100	ppm
Co	9.7	[N]	2	ppm
Cr	5.4	[O]	2	ppm

Hf	.30	Y	<.001
Mo	.59	La	<.001
Ni	Balance	Ce	<.002
Re	1.5
Ta	8.3
Ti	.71
W	7.8

	Zr	<10	ppm

Ag	<.4	ppm
Bi	<.2	ppm
Ga	<10	ppm
Ca	<25	ppm
Pb	<.5	ppm
Se	<.5	ppm
Te	<.2	ppm
Tl	<.2	ppm
Sn	<2	ppm
Sb	<1	ppm
As	<1	ppm
Zn	<1	ppm
Hg	<2	ppm
Cd	<.2	ppm
Ge	<1	ppm
Au	<.5	ppm
In	<.2	ppm
Na	<10	ppm
K	<5	ppm
Ba	<10	ppm
P	6	ppm
U	<.5	ppm
Th	<1	ppm

TABLE 3

CMSX ®-8 Heat - 5V0460
Molds 925/926 - RR SCFO [Indy] - LA 11832 (Joliet/CM 366)
Fully Heat Treated - Solution + Double Age [DL-10s]

Creep-Rupture

		Rupture Life,	%	%	1%	2%
Test Condition	ID	hrs	Elong	RA	Creep	Creep

1562° F./94.4 ksi	A925	211.9	17.5	21.5	7.3	39.1
[850° C./651 Mpa]	B926	157.1	16.4	22.8	2.3	23.2
1600° F./65.0 ksi	B925	1072.0	27.4	33.5	482.8	631.5
[871° C./448 Mpa]	C926	983.5	26.8	33.0	407.8	536.4
1800° F./36.0 ksi	C925	200.2	35.0	43.3	109.7	125.1
[982° C./248 Mpa]	E926	246.7	44.6	46.0	120.0	140.1
1850° F./38.0 ksi	E925	86.0	37.2	38.6	39.7	46.6
[1010° C./262 Mpa]	H926	65.9	41.4	44.0	28.6	35.6
1900 F/25.0 ksi	H925	214.7	38.6	39.4	82.0	105.0
1038° C./172 Mpa]	J926	199.6	33.2	39.5	65.3	93.7
1904° F./21.0 ksi	J925	362.4	30.0	37.5	141.3	182.6
[1040° C./145 Mpa]	K926	359.1	33.1	34.8	164.2	194.6
1950° F./18.0 ksi	L925	481.1	31.4	34.9	194.1	246.1
[1066° C./124 Mpa]	M926	449.6	40.0	38.9	166.1	211.5

Stress-Rupture

Test Condition	ID	Rupture Life, hrs	(4D) % Elong	% RA

2000° F./12.0 ksi	N925	1983.2	13.0	37.9
[1093°/83 Mpa]	R926	1979.9	24.8	33.0
2050° F./15.0 ksi	R925	275.5	24.5	38.3
[1121°/103 Mpa]	L926	285.4	22.9	40.4

Alternate Heat Treatment (Tmax 2408° F.)

1800° F./36.0 ksi	D925	249.0	43.1	44.0	114.5	134.8
[982° C./248 Mpa]
2050° F./15.0 ksi	A926	271.8	13.6	38.1	—	—
[1121°/103 Mpa]

Phase stability is surprisingly good with absolutely negligible TCP phases apparent in the post-test creep/stress rupture bars examined to date (FIGS. 5-16 inclusive and 22-23 inclusive).
Recent work has shown it is possible to adequately solution/homogenize heat treat a single crystal test bar in the alloy (FIG. 17), using a shortened cycle—2 hrs/2365° F. (1296° C.)+2 hrs/2385° F. (1307° C.)+2 hrs/2395° F. (1313° C.)+2 hrs/2403° F. (1317° C.)+8 hrs/2408° F. (1320° C.) AC (8 hrs shorter). Limited creep/stress-rupture properties at critical conditions using this shorter solution/homogenization heat treatment show very similar results to the original solution heat treatment condition (Table 3 and 4) and good phase stability [no TCP phases] (FIGS. 19 & 20).
Burner rig dynamic, cyclic oxidation and hot corrosion (sulfidation) testing is currently scheduled at a major turbine engine company.
Creep/stress-rupture data for fully heat treated solution/homogenized and double aged (DL-10s) test specimens for the disclosed alloys are presented in Table 4.

TABLE 4

CMSX ®-8 Heat 5V0460
Heat 5V0460 - Mold 54275 - HP2 Solid Turbine
Blades RR SCFO [Indy] - LA11865 (Joliet 9220/CM-373)
Fully Heat Treated - Solution + double age - 2050° F. Primary age

Stress-Rupture MFB Mini Bars [0.070″ø gage] (LLE)

			% (4D)	%
Test Condition	ID	Rupture Life, hrs	Elong	RA

1562° F./94.4 ksi	54275A-B	449.0	16.3	18.7
[850° C./651 MPa]	54275B-B	359.8	18.7	19.9
1800° F./36.0 ksi	54275E-B	223.4	43.1	45.6
[982° C./248 MPa]	54275H-B	219.1	45.1	46.9
1850° F./38.0 ksi	54275I-B	74.2	46.2	47.8
[1010° C./262 MPa]	54275J-B	76.7	39.2	43.8
1900° F./25.0 ksi	54275K-B	181.8	41.2	48.5
[1038° C./172 MPa]	54275L-B	190.8	41.8	38.9
1904° F./21.0 ksi	54275R-B	354.0	43.9	40.2
[1040° C./45 MPa]	54275O-B	599.3	39.2	45.7
1950° F./18.0 ksi	54275T-B	410.1	27.9	48.8
[1066° C./124 MPa]	54275U-B	420.6	39.1	41.1
2050° F./15.0 ksi	54275X-B	287.5	26.3	32.7
[1121° C./103 Mpa]	54275Y-B	205.8	22.7	25.1

MFB Mini Flats [0.020″ Thick Gage] (LTE)

Test Condition	ID	Rupture Life, hrs	% Elong

1800° F./30.0 ksi	54275A-F	490.7	41.1
[982° C./207 MPa]	54275B-F	446.0	28.8
	54275E-F	437.5	24.2
	54275H-F	381.9	31.6
1904° F./21.0 ksi	54275I-F	404.0	36.4
[1040° C./145 MPa]	54275J-F	325.1	28.6
	54275K-F	312.1	24.5
	54275L-F	341.1	26.6

Mini-flat bar stress-rupture testing was performed on single crystal solid turbine blades 10 (FIG. 21) cast from alloys as disclosed herein that have facility to machine mini-bar specimens 15 and mini-flat specimens 20.
A Larson-Miller stress-rupture graph (FIG. 18) shows CMSX®-8 alloy has surprisingly good stress-rupture life properties, from machined-from-blade (MFB) mini-flat (0.020″ (0.508 mm) gage thickness) specimens, that are close to those of a CMSX-4® alloy.
The embodiments disclosed herein are non-limiting examples that are provided to illustrate and facilitate a better understanding, the scope of the invention being defined by the appending claims as properly construed under the patent laws, including the doctrine of equivalents.

Claims

What is claimed is:

1. A nickel-base superalloy for single crystal casting, comprising:

5.60% to 5.80% aluminum by weight;

9.4% to 9.9% cobalt by weight;

4.9% to 5.5% chromium by weight;

0.08% to 0.35% hafnium by weight;

0.50% to 0.70% molybdenum by weight;

1.4% to 1.6% rhenium by weight;

8.1% to 8.5% tantalum by weight;

0.60% to 0.80 titanium by weight;

7.6 to 8.0% tungsten by weight; and

the balance comprising nickel and minor amounts of incidental elements, the total amount of incidental elements being about 1% or less.

2. A nickel-base superalloy for single crystal casting according to claim 1, in which the incidental elements are present at maximum amounts of 100 ppm carbon, 0.04% silicon, 0.01% manganese, 3 ppm sulfur, 30 ppm phosphorous, 30 ppm boron, 0.10% niobium, 150 ppm zirconium, 0.01% copper, 0.15% iron, 0.10% vanadium, 0.10% ruthenium, 0.15% platinum, 0.15% palladium, 200 ppm magnesium, 5 ppm nitrogen, 5 ppm oxygen, and other trace elements present in amounts of about 25 ppm or less.

3. A nickel-base superalloy for single crystal casting according to claim 1, in which the trace elements are present at maximum amounts of 2 ppm silver, 0.2 ppm bismuth, 10 ppm gallium, 25 ppm calcium, 1 ppm lead, 0.5 ppm selenium, 0.2 ppm tellurium, 0.2 ppm thallium, 10 ppm tin, 2 ppm antimony, 2 ppm arsenic, 5 ppm zinc, 2 ppm mercury, 2 ppm cadmium, 2 ppm germanium, 2 ppm gold, 2 ppm indium, 20 ppm sodium, 10 ppm potassium, 20 ppm barium, 30 ppm phosphorous, 2 ppm uranium, and 2 ppm thorium.

4. A nickel-base superalloy for single crystal casting according to claim 1, in which sulfur is present at a maximum of 0.5 ppm, and lanthanum and/or yttrium are added in an amount targeted to achieve from about 5 ppm to about 80 ppm of total lanthanum and yttrium in a single crystal casting.

5. A nickel-base superalloy for single crystal casting according to claim 1, in which carbon is present in an amount of from 0.02% to 0.05%, and boron is present in an amount of from 40 ppm to 100 ppm.

6. A nickel-base superalloy for single crystal casting according to claim 1, having a density of about 8.90 gms/cc (kg/dm³) or less.

7. A nickel-base superalloy for single crystal casting according to claim 1, having a density of about 8.85 gms/cc (kg/dm³).

8. A single crystal component cast from an alloy according to claim 1.

9. A single crystal component according to claim 8 that is a gas turbine component.

10. A single crystal component according to claim 8 that is a turbine blade, a vane, or a seal segment for a gas turbine.