Intermediate strength alloys for high temperature service in liquid-salt cooled energy systems

Information

  • Patent Grant
  • 9683280
  • Patent Number
    9,683,280
  • Date Filed
    Friday, January 10, 2014
    10 years ago
  • Date Issued
    Tuesday, June 20, 2017
    7 years ago
Abstract
An alloy consists essentially of, in terms of weight percent: 6 to 8.5 Cr, 5.5 to 13.5 Mo, 0.4 to 7.5 W, 1 to 2 Ti, 0.7 to 0.85 Mn, 0.05 to 0.3 Al, up to to 0.1 Co, 0.08 to 0.5 C, 1 to 5 Ta, 1 to 4 Nab, 1 to 3 Hf, balance Ni. The alloy is characterized by, at 850° C., a yield strength of at least 36 Ksi, a tensile strength of at least 40 Ksi, a creep rupture life at 12 Ksi of at least 72.1 hours, and a corrosion rate, expressed in weight loss [g/(cm2sec)]×10−11 during a 1000 hour immersion in liquid FLiNaK at 850° C., in the range of 8 to 25.
Description
CROSS-REFERENCE TO RELATED APPLICATIONS

This patent application is related to U.S. patent application Ser. No. 13/834,985 entitled “High Strength Alloys for High Temperature Service in Liquid-Salt Cooled Energy Systems” filed on Mar. 15, 2013, the entire disclosure of which is incorporated herein by reference. Moreover, this patent application is related to U.S. patent application Ser. No. 13/958,672 entitled “Creep-Resistant, Cobalt-Containing Alloys for High Temperature, Liquid-Salt Heat Exchanger Systems” filed on Aug. 5, 2013, the entire disclosure of which is incorporated herein by reference. Moreover, this patent application is related to U.S. patent application Ser. No. 13/962,197 entitled “Creep-Resistant, Cobalt-Free Alloys for High Temperature, Liquid-Salt Heat Exchanger Systems” filed on Aug. 8, 2013, the entire disclosure of which is incorporated herein by reference.


BACKGROUND OF THE INVENTION

An ever-increasing demand for higher system thermal efficiency has necessitated the operation of power generation cycles and heat conversion systems for chemical processes at progressively higher temperatures. As system operating temperatures are increased, fewer materials with acceptable mechanical properties and environmental compatibility are known. This dearth of materials is particularly acute in applications at temperatures above 700° C. especially when accompanied by significant stress levels. Liquid fluoride salts are favored as heat transfer media at these high temperatures because of their high thermal capacity and low vapor pressure. There is, therefore, a need for fluoride salt compatible structural alloys for high-temperature heat transfer applications in order to enable increased thermal efficiency of energy conversion and transport systems thereby reducing system costs as well as reducing the waste heat rejected to the environment.


Fluoride salt cooled High temperature Reactors (FHRs) potentially have attractive performance and safety attributes. Defining features of FHRs include coated particle fuel, low-pressure fluoride salt cooling, and high-temperature heat production. The FHR heat transfer technology base is derived primarily from earlier molten salt reactors and their coated particle fuel is similar to that developed for high-temperature helium-cooled reactors. The excellent heat transfer characteristics of liquid fluoride salts enable full passive safety, at almost any power scale, thereby enabling large power output reactors with less massive piping and containment structures, and consequent economies of scale. FHRs potentially have improved economics, increased safety margins, and lower water usage characteristics than conventional water-cooled reactors.


The fuel and coolants for FHRs are suitable for operation at temperatures well in excess of the upper temperature limits of available structural alloys. A limiting factor in achieving the highest possible FHR core outlet temperatures, and thus thermal efficiency, is the availability of structural alloys having sufficient creep strength at the required temperatures combined with suitable fluoride salt chemical compatibility as well as ease of fabrication and joining. Hastelloy® N (trademark owned by Haynes International, Inc.) (also known as Alloy N and INOR-8), developed at Oak Ridge National laboratory (ORNL) in the 1950s and 1960s, is currently a leading candidate FHR structural alloy for operations below 700° C. Hastelloy® N is limited to use in low stress applications to a maximum temperature of about 704° C. due to insufficient creep strength at higher temperatures, is limited to use in high stress applications such as steam generator tubes to about 600° C. due to insufficient creep strength at higher temperatures, is not fully qualified to current code requirements for high temperature reactors, and is challenging to fabricate due to its work hardening characteristics. There is therefore a need for corrosion-resistant nickel-based structural alloys designed to possess good creep resistance in liquid fluorides at higher temperatures in order to provide substantial improvements in FHR economics and performance. Calculations reveal that a net thermal efficiency of greater than 50% (as compared to about 33% net thermal efficiency of existing reactors) would be likely for FHRs using a high temperature structural alloy with concurrent reductions in capital costs, waste generation, fissile material requirements, and cooling water usage.


Other applications for these alloys include concentrated solar power (CSP), and processing equipment for fluoride environments. Molten-salt power towers are envisioned as operating in excess of 650° C. to achieve efficiency and cost targets. Temperatures of up to 700° C. are anticipated with the use of commercial supercritical steam turbines, up to 800° C. with the use of supercritical CO2 Brayton cycle system, and even higher temperatures using open air Brayton cycle systems. Molten salts allow for the storage of solar energy and thus, the decoupling of solar energy collection from electricity generation. At the higher temperatures, molten fluoride salts offer the advantages of high thermal capacity, high heat transfer, and low vapor pressure. The development of materials with acceptable mechanical and molten salt corrosion resistance will allow for achieving the desired efficiency and cost targets.


Development of a high temperature structural alloy tailored to the specific high temperature strength and liquid salt corrosion resistance needs of liquid fluoride salt cooled-energy systems (especially FHRs) is contemplated to be of critical importance to ensuring feasibility and performance thereof. Simultaneously achieving creep resistance and liquid fluoride salt resistance at higher temperatures is challenging because conventional additions of certain alloying elements for achieving improved creep resistance and resistance to oxidation in air are detrimental to liquid fluoride salt resistance.


In general, conventional Ni-based alloys are strengthened through a combination of solid solution strengthening and precipitation strengthening mechanisms with the latter needed to achieve higher strengths at higher temperatures. In one class of Ni-based superalloys, primary strengthening is obtained through the homogeneous precipitation of ordered, L12 structured, Ni3(Al,Ti,Nb)-based intermetallic precipitates that are coherently embedded in a solid solution face centered cubic (FCC) matrix. In another class of Ni-based alloys, creep resistance is achieved through the precipitation of fine carbides (M23C6, M7C3, M6C where M is primarily Cr with substitution of Mo, W, for example) and carbonitrides (M(C, N) where M is primarily Nb, or Ti, for example) within the matrix, and larger carbides on grain boundaries to prevent grain boundary sliding. Moreover, high temperature oxidation resistance in these alloys is obtained through additions of Cr and Al. Existing data (shown in FIG. 1) on liquid fluoride salt resistance of Ni-based alloys show that alloys containing aluminum and substantial amounts of chromium have lower resistance to liquid fluoride salt. Commercial nickel-based alloys with high strengths typically contain significant amounts of Cr (greater than 15 wt. % Cr) making them unsuitable for use in contact with liquid fluoride salts. Compositions (in weight %) of several commercially produced Ni-based alloys are shown in Table 1.


Hastelloy® N is an alloy that was designed to balance resistance to liquid fluoride salt corrosion with good creep properties at temperatures up to 704° C. This alloy is a Ni—Mo alloy containing additional alloying elements with solid solution strengthening being the primary strengthening mechanism; Hastelloy® N does not have γ′ precipitation strengthening. Its nominal composition is given as

71Ni-7Cr-16Mo-5Fe*-1Si*-0.8Mn*-0.2Co*-0.35Cu*-0.5W*-0.35Al+Ti*-0.08C*

where * indicates maximum allowed content of the indicated elements. Hastelloy® N generally consists of the following elements to provide the corresponding benefits:


Chromium: Added to ensure good oxidation resistance but minimized to keep liquid fluoride salt corrosion within acceptable limits. Also provides solid solution strengthening. Too much addition results in excessive attack by liquid fluoride salts.


Molybdenum: Principal strengthening addition for solid solution strengthening, provides good resistance to liquid fluoride salt, and results in lower interdiffusion coefficients. Also is the primary constituent in M6C carbides. Too much addition can result in the formation of undesirable, brittle intermetallic phases.


Iron: Minimizes cost of alloy. Provides solid solution strengthening. Too much addition can destabilize austenitic matrix and decrease resistance to liquid fluoride salt.


Manganese: Stabilizes the austenitic matrix phase. Provides solid solution strengthening.


Silicon: Assists in high temperature oxidation resistance, a maximum of 1% Si may be added.


Carbon, Nitrogen: Required for the formation of carbide and/or carbonitride phases that can act as grain boundary pinning agents to minimize grain growth and to provide resistance to grain boundary sliding. Fine precipitation of carbide and/or carbonitride phases can increase high temperature strength and creep resistance.


Copper: Stabilizes the austenitic matrix, provides solid solution strengthening.


Cobalt: Provides solid solution strengthening. Co should not be present in alloys exposed to high neutron fluxes or whose corrosion products are exposed to high neutron fluxes, since these are subject to activation.


Tungsten: Provides solid solution strengthening and decreases average interdiffusion coefficient. Too much W can result in the formation of brittle intermetallic phases that can be deleterious to processability.


Aluminum+Titanium are not desirable in Hastelloy® N, in order to minimize corrosion by liquid salt. Combined wt. % of Al+Ti is typically kept to less than 0.35.



FIG. 1 shows effects of alloying element additions on the depth of corrosion of Ni-alloys in 54.3LiF-41.0KF-11.2NaF-2.5UF4 (mole percent) in a thermal convention loop operated between 815 and 650° C. (smaller depth of corrosion is better).



FIG. 2 shows the equilibrium phase fractions in Hastelloy® N as a function of temperature. Note that solid solution strengthening and some carbide strengthening (through M6C) are the primary strengthening mechanisms active in Hastelloy® N. This limits the strength and creep resistance of Hastelloy® N at high temperatures and restricts its useful temperatures to less than about 704° C. Components such as power cycle heat exchangers need to withstand large pressure differences between salt on one side of the heat exchanger wall and a gaseous working fluid at higher pressures on the other side. Such components hence need materials with high temperature strength greater than that of Hastelloy® N along with good resistance to salt, and good oxidation resistance.


BRIEF SUMMARY OF THE INVENTION

In accordance with one aspect of the present invention, the foregoing and other objects are achieved by an alloy consisting essentially of, in terms of weight percent: 6 to 8.5 Cr, 5.5 to 13.5 Mo, 0.4 to 7.5 W, 1 to 2 Ti, 0.7 to 0.85 Mn, 0.05 to 0.3 Al, up to 0.1 Co, 0.08 to 0.5 C, 1 to 5 Ta, 1 to 4 Nb, 1 to 3 Hf, balance Ni. The alloy is characterized by, at 850° C., a yield strength of at least 36 Ksi, a tensile strength of at least 40 Ksi, a creep rupture life at 12 Ksi of at least 72.1 hours, and a corrosion rate, expressed in weight loss [g/(cm2sec)]×10−11 during a 1000 hour immersion in liquid FLiNaK at 850° C., in the range of 8 to 25.





BRIEF DESCRIPTION OF THE DRAWINGS


FIG. 1 is a combination table and bar graph showing effects of alloying element additions on the depth of corrosion of Ni-alloys in 54.3LiF-41.0KF-11.2NaF-2.5UF4 (mole percent) in a thermal convention loop operated between 815 and 650° C.



FIG. 2 is a graph showing phase equilibria for a typical composition of Hastelloy® N as a function of temperature (nitrogen and boron are not included in the calculations).



FIG. 3 is a graph showing phase equilibria for Alloy 3 as a function of temperature (nitrogen and boron are not included in the calculations).



FIG. 4 is an expanded view of a portion of the graph shown in FIG. 3 to show details.



FIG. 5 is a graph showing phase equilibria for Alloy 4 as a function of temperature (nitrogen and boron are not included in the calculations).



FIG. 6 is an expanded view of a portion of the graph shown in FIG. 5 to show details.



FIG. 7 is a graph showing phase equilibria for Alloy 5 as a function of temperature (nitrogen and boron are not included in the calculations).



FIG. 8 is an expanded view of a portion of the graph shown in FIG. 7 to show details.



FIG. 9 is a graph showing phase equilibria for Alloy 20 as a function of temperature (nitrogen and boron are not included in the calculations).



FIG. 10 is an expanded view of a portion of the graph shown in FIG. 9 to show details.



FIG. 11 is a graph showing phase equilibria for Alloy 22 as a function of temperature (nitrogen and boron are not included in the calculations).



FIG. 12 is an expanded view of a portion of the graph shown in FIG. 11 to show details.



FIG. 13 is a graph showing phase equilibria for Alloy 24 as a function of temperature (nitrogen and boron are not included in the calculations).



FIG. 14 is an expanded view of a portion of the graph shown in FIG. 13 to show details.





For a better understanding of the present invention, together with other and further objects, advantages and capabilities thereof, reference is made to the following disclosure and appended claims in connection with the above-described drawings.


DETAILED DESCRIPTION OF THE INVENTION

New, essentially Fe-free, solid-solution-strengthened alloys having improved high temperature strength and creep resistance; general composition limits are shown in Table 2. The primary strengthening in the new alloys is achieved through the precipitation of carbides along with solid solution strengthening. Moreover, the new alloys exhibit an advantageously lower average interdiffusion coefficient in the matrix. The skilled artisan will recognize that a lower interdiffusion rate results in, at high temperatures, lower coarsening rate of carbides, improved creep properties, lower oxidation rate, and lower corrosion rate.


Computational design was used to ensure that formation of brittle intermetallic phases that form in the new alloys is very low or zero weight % in the operating temperature range of contemplated greatest interest (750 to 950° C.). In the alloys, small amounts of carbide formers such as Ti, Nb, Hf, and Ta have been added to form carbides and the carbon levels have been increased as compared to Hastelloy® N. Carbides such as, for example, M6C and MC, or a combination thereof are present in these alloys in addition to the M6C carbides that are formed in Hastelloy® N.


The precipitate strengthened alloys described herein provide the higher strength required for applications for which the solid solution strengthened alloys have insufficient strength, and also provide improved creep strength. One disadvantage with conventional carbide strengthened alloys is that the strength decreases with time at temperature due to the coarsening of the carbide precipitates. The rate of loss of strength is directly related to the rate of growth of precipitates, which increases with increase in temperature (which also results in an increase in interdiffusion coefficients). The addition of sufficient amount of Mo, W, and/or Ta to the alloys of the present invention ensures that the interdiffusion coefficient is kept as low as reasonably possible and the coarsening rates are low, thus retaining properties for an extended period of time.


Broadest constituent ranges for alloys of the present invention are set forth in Table 2. Some examples thereof are set forth in Table 3, with Hastelloy® N for comparison. It is contemplated that alloys of the present invention may contain up to 5% Fe with concomitant reduction in some beneficial properties, such as creep resistance and oxidation resistance. Moreover, particularly in applications where the alloy is subject to nuclear radiation, cobalt may be eliminated to reduce activation with a small but concomitant reduction in strength and creep properties.


EXAMPLES

Alloys 3, 4, 5, 20, 22, and 24, shown in Table 3 were made using well known, conventional methods. Vacuum arc cast ingots were annealed at 1200° C. in an inert gas environment (vacuum can also be used). The ingots were then hot-rolled into plates for mechanical testing. A solution annealing treatment was performed at 1150° C. for 1 hour. Thus, all the alloys can be cast, heat-treated, and mechanically processed into plates and sheets. The skilled artisan will recognize that other, conventional heat-treatment schedules can be used.



FIGS. 3-14 show the results from equilibrium calculations obtained from the computational thermodynamics software JMatPro v 6.2. Actual compositions were used for all the calculations.


Table 4 shows equilibrium wt. % of phases present in alloys at 850° C. It is essential that an alloy have M6C type carbides and at least one of MC type carbides and Ni5M type precipitates for optimum creep resistance. Small, finely dispersed carbides produced by heat-treatment improve creep resistance and are preferred over large carbides formed during solidification. Total precipitate phases must be present in a range of 4.0 to 10 wt. %. M6C type carbides must be present in a range of 1 to 8 wt. %. MC type carbides can be present in a range of up to 3.5 wt. %. Ni5M type precipitates can be present in a range of up to 3 wt. %. It is contemplated that more than 3 wt. % Ni5M type precipitates may be potentially deleterious to mechanical properties.


Yield and tensile strengths have been measured at 850° C. and compared with the baseline properties of Hastelloy® N and are shown in Table 5. Note that the yield strengths of the new alloys at 850° C. in the solution annealed condition are 2.5-26% better than that of Hastelloy® N. Typical yield strengths of alloys of the present invention are contemplated to be at least 36 Ksi, preferably at least 40 Ksi. Typical tensile strengths of alloys of the present invention are contemplated to be at least 40 Ksi, preferably at least 50 Ksi.


Creep rupture life has been measured in the solution annealed condition at 850° C. at a stress level of 12 Ksi with the new alloys showing improvements in rupture lives of about 1812% to 4774%, as shown in Table 6. Creep rupture lives of alloys of the present invention are contemplated to be at least 72 hours, preferably at least 100 hours.


Resistances to liquid salt corrosion were measured by placing the alloy specimens of measured dimensions and weight in sealed molybdenum capsules in contact with a fixed amount of FLiNaK, a liquid salt heat exchange medium. The molybdenum capsules were enclosed in outer capsule to minimize high temperature air oxidation and heated in a furnace at 850° C. for 1,000 hours. After exposure, the capsules were opened and the specimens cleaned, weighed and their dimension measured. Corrosion resistance to liquid fluoride salt was evaluated based on normalized weight change and metallography and scanning electron microscopy. Results presented in Table 7 demonstrate that these alloys all have corrosion rates slightly higher than that of Hastelloy® N in these isothermal tests but with significantly improved mechanical properties. Thus a balance has been struck between improved mechanical properties and resistance to attack by liquid fluoride salt. Note that the aluminum and chromium has been kept at minimum required levels without adversely affecting the oxidation resistance and the salt resistance of these alloys. Typical corrosion rates of alloys of the present invention, expressed in weight loss [g/(cm2sec)]×10−11 during a 1000 hour immersion in liquid FLiNaK at 850° C., are contemplated to be in the range of about 8 to about 25. Thus a balance has been struck between improved mechanical properties and resistance to attack by liquid fluoride salt.


Table 8 shows the relationship between the susceptibility to corrosion of the alloys shown by liquid fluoride salts, specifically FLiNaK with the Mo Equivalent, defined as







Mo





Equivalent

=


%





Mo

+

1.15
×


183.84






(

Atomic





Weight





of





W

)



95.95






(

Atomic





Weight





of





Mo

)



×
%





W







where % refers to atomic percent of the element present in the alloy. 183.84 is the atomic wt. of W 95.95 is the atomic wt. of Mo. It has been observed that for these alloys the Mo Equivalent should be in the range of 5 to 12 for good resistance to liquid fluoride salts, specifically FLiNaK.


Table 8 shows the corrosion susceptibility index which quantifies the susceptibility to corrosion of the alloys shown in Table 3 by liquid fluoride salts, specifically FLiNaK. For this purpose, we define the corrosion susceptibility index as







C





S





I

=



%





Al

+

%





Cr

+

%





Ti

+

%





Nb

+

%





Hf

+

%





Ta




%





Ni

+

%





Fe

+

%





Co

+

%





Mn

+

%





Mo

+

%





W

+

%





Re

+

%





Ru








where % refers to atomic percent of the element present in the alloy. It has been observed that for these alloys, CSI should be no less than than about 0.1 and no greater than about 0.2 in addition to maintaining the elements in the preferred ranges. This results in the optimum combination of mechanical properties (high temperature strength and creep resistance) and resistance to fluoride salts.


Tables 1-8 follow.


While there has been shown and described what are at present considered to be examples of the invention, it will be obvious to those skilled in the art that various changes and modifications can be prepared therein without departing from the scope of the inventions defined by the appended claims.









TABLE 1







Compositions of several commercial Ni-based alloys (in weight %).






















Alloy
C
Si
Mn
Al
Co
Cr
Cu
Fe
Mo
Nb
Ni
Ta
Ti
W
Zr

























X750
0.03
0.09
0.08
0.68
0.04
15.7
0.08
8.03

0.86
Bal
0.01
2.56




Nimonic 80A
0.08
0.1
0.06
1.44
0.05
19.6
0.03
0.53


Bal

2.53




IN 751
0.03
0.09
0.08
1.2
0.04
15.7
0.08
8.03

0.86
Bal
0.01
2.56




Nimonic 90
0.07
0.18
0.07
1.4
16.1
19.4
0.04
0.51
0.09
0.02
Bal

2.4

0.07


Waspaloy
0.03
0.03
0.03
1.28
12.5
19.3
0.02
1.56
4.2

Bal

2.97

0.05


Rene 41
0.06
0.01
0.01
1.6
10.6
18.4
0.01
0.2
9.9

Bal

3.2




Udimet 520
0.04
0.05
0.01
2.0
11.7
18.6
0.01
0.59
6.35

Bal

3.0




Udimet 720
0.01
0.01
0.01
2.5
14.8
15.9
0.01
0.12
3.0
0.01
Bal

5.14
1.23
0.03


Alloy 617
0.07
0
0
1.2
12.5
22
0
1
9
0
54
0
0.3
0
0
















TABLE 2







Compositions of new alloys (analyzed compositions in wt. %)











Element
Minimum wt. %
Maximum wt. %















Cr
6
8.5



Mo
5.5
13.5



W
0.4
7.5



Ti
1
2



Mn
0.7
0.85



Al
0.05
0.3



Co
<0.005
0.1



C
0.08
0.5



Ta
1
5



Nb
1
4



Hf
1
3











Fe
Essentially 0




Ni
Balance

















TABLE 3





Compositions of new alloys compared to Hastelloy ® N (analyzed compositions in wt. %)























Alloy
Ni
Fe
Al
Co
Cr
Mn
Mo
Ti





Hastelloy ® N*
68.7
5

0.2
7
0.8
16
0


Alloy 3
73.87
0
0.1
0.04
6.9
0.77
12.91
1.18


Alloy 4
74.02
0
0.1
0.0298
6.88
0.78
12.93
1.19


Alloy 5
78.85
0
0.09
0.02
6.7
0.79
8.17
1.18


Alloy 20
72.2892
0.01
0.09
0.01
7.09
0.77
7.48
1.22


Alloy 22
70.57
0
0.08
0.08
8.23
0.75
5.81
1.19


Alloy 24
71.01
0.01
0.11
0.01
6.83
0.76
5.92
1.15





Alloy
Nb
Hf
Ta
W
C
B**
N**
Total





Hastelloy ® N*

0
0
0.5
0.08
0.01

100


Alloy 3
1.06
1.16
1.19
0.59
0.23
0
0.0005
100


Alloy 4
1.06
1.13
1.18
0.6
0.1
0
0.0002
100


Alloy 5
1.09
1.16
1.18
0.52
0.25
0
0.0002
100


Alloy 20
1.17
2.77
1.22
5.67
0.21
0
0.0005
100


Alloy 22
3.76
1.15
1.2
6.99
0.19
0
0.0012
100


Alloy 24
1.15
1.13
4.82
6.88
0.22
0
0.0037
100





*Hastelloy ® N also contains 1 Si, 0.35 Cu, 0.5 max of Al + Ti


**Boron and Nitrogen are not included in the equilibrium calculations













TABLE 4







Equilibrium wt. % of Phases Present in Alloys at 850° C.














Wt. %
Wt. % M6C
Wt. % MC
Total
Wt. % Ni5M
Total Precipitate


Alloy
γ
Precipitates
Precipitates
Carbides
Precipitates
Phases
















Hastelloy ® N
98.77
1.23
0
1.23
0
1.23


Alloy 3
90.68
7.54
0.66
8.20
1.12
9.22


Alloy 4
93.37
4.0
0
4.0
2.63
6.63


Alloy 5
92.83
5.78
1.39
7.17
0
7.17


Alloy 20
95.91
1.11
2.98
4.09
0
4.09


Alloy 22
95.93
2.31
1.76
4.07
0
4.07


Alloy 24
93.89
4.52
1.59
6.11
0
6.11
















TABLE 5







Yield and Tensile Strengths of Alloys at 850° C. and


Improvement in Yield Strength over the baseline alloy.













Yield
Tensile
% Improvement



Alloy
Strength
strength
in Yield Strength
















Hastelloy ® N
35.29
45.70
0



Alloy 3
41.67
49.93
18.1



Alloy 4
37.18
50.93
5.4



Alloy 5
36.18
40.30
2.5



Alloy 20
41.93
53.27
18.8



Alloy 22
44.35
57.27
25.7



Alloy 24
44.35
55.27
25.7

















TABLE 6







Creep rupture lives of alloys at 850° C., at a stress of 12 Ksi and


improvement over the baseline alloy.













% Improvement in



Alloy
Creep Rupture Life
creep rupture life















Hastelloy ® N
3.77
0




(average of 3 tests)



Alloy 3
183.7
4773



Alloy 4
109
2791



Alloy 5
72.1
1812



Alloy 20
116
2977



Alloy 22
128.8
3316



Alloy 24
138.2
3566

















TABLE 7







Corrosion Rate (Weight Loss) Measured During a 1000 hour


immersion in liquid FLiNaK at 850° C.










Alloy
Corrosion rate [g/(cm2sec)]10−11














Hastelloy ® N
1.21



Alloy 3
20.34



Alloy 4
21.87



Alloy 5
22.99



Alloy 20
11.28



Alloy 22
10.43



Alloy 24
16.06

















TABLE 8





Composition of alloys in at. % and the calculation of Mo Equivalent and Corrosion Susceptibility Index (CSI)























Alloy
Ni
Fe
Al
Co
Cr
Mn
Mo
Ti





Hastelloy ® N*
75.735
4.443
0
0.157
7.473
0.594
10.34
0


Alloy 3
77.8959
0
0.229
0.0421
8.213
0.867
8.328
1.526


Alloy 4
78.4595
0
0.231
0.0315
8.232
0.883
8.385
1.547


Alloy 5
81.492
0
0.202
0.02
7.816
0.872
5.166
1.495


Alloy 20
78.3326
0.01139
0.212
0.01
8.672
0.891
4.959
1.621


Alloy 22
76.516
0
0.189
0.086
10.07
0.869
3.854
1.582


Alloy 24
78.2414
0.01158
0.264
0.01
8.495
0.895
3.991
1.554



















Alloy
Nb
Hf
Ta
W
C
Mo Equ.
CSI






Hastelloy ® N*
0
0
0
0.02
0.154
10.38
0.081861



Alloy 3
0.706
0.402
0.407
0.199
1.185
8.77
0.1315



Alloy 4
0.71
0.394
0.406
0.203
0.518
8.83
0.1310



Alloy 5
0.712
0.394
0.396
0.172
1.263
5.55
0.1256



Alloy 20
0.801
0.987
0.429
1.962
1.112
9.28
0.1476



Alloy 22
2.575
0.41
0.422
2.42
1.007
9.19
0.1821



Alloy 24
0.801
0.409
1.723
2.42
1.185
9.32
0.1548








Claims
  • 1. An alloy for use in components in contact with liquid fluorides, consisting essentially of, in terms of weight percent: Cr: 6 to 8.5,Mo: 5.5 to 13.5,W: 0.4 to 7.5,Ti: 1 to 2,Mn: 0.7 to 0.85,Al: 0.05 to 0.3,Co: 0 to 0.1,C: 0.08 to 0.5,Ta: 1 to 5,Nb: 1 to 4,Hf: 1 to 3,Fe: ≦0.01,Ni: balance,with Al+Ti≦2.3 wt. %;and said alloy being characterized byi) at alloy temperatures of 850° C., a yield strength of at least 36 Ksi, a tensile strength of at least 40 Ksi, a creep rupture life at 12 Ksi of at least 72.1 hours, and a corrosion rate of 8×10−11 g/cm2s to 25×10−11 g/cm2s of weight loss during a 1000 hour immersion in liquid FLiNaK at 850° C.;ii) at alloy temperatures of 850° C., a matrix consisting of γ and 4.0 to 10 wt. % total precipitates, said total precipitates consisting of at least one M6C type carbide and at least one additional precipitate selected from the group consisting of MC type carbides and Ni5M type precipitates;iii) said alloy possessing an Mo Equivalent of no less than 5, wherein,
  • 2. An alloy in accordance with claim 1 wherein the range of Cr is 6.7 to 8.3 weight percent.
  • 3. An alloy in accordance with claim 1 wherein the range of Mo is 5.81 to 12.93 weight percent.
  • 4. An alloy in accordance with claim 1 wherein the range of W is 0.52 to 6.99 weight percent.
  • 5. An alloy in accordance with claim 1 wherein the range of Ti is 1.15 to 1.22 weight percent.
  • 6. An alloy in accordance with claim 1 wherein the range of Mn is 0.75 to 0.79 weight percent.
  • 7. An alloy in accordance with claim 1 wherein the range of Al is 0.08 to 0.11 weight percent.
  • 8. An alloy in accordance with claim 1 wherein the range of Co is 0.01 to 0.08 weight percent.
  • 9. An alloy in accordance with claim 1 wherein the range of Ta is 1.18 to 4.82 weight percent.
  • 10. An alloy in accordance with claim 1 wherein the range of Nb is 1.06 to 3.76 weight percent.
  • 11. An alloy in accordance with claim 1 wherein the range of Hf is 1.13 to 2.77 weight percent.
  • 12. An alloy in accordance with claim 1 wherein the range of C is 0.1 to 0.25 weight percent.
  • 13. An alloy in accordance with claim 1 wherein sad alloy is further characterized by 1 to 8 wt. % M6C type carbides.
  • 14. An alloy in accordance with claim 1 wherein said alloy is further characterized by up to 3.5 wt. % MC type carbides.
  • 15. An alloy in accordance with claim 1 wherein said alloy is further characterized by up to 3 wt. % Ni5M type precipitates.
STATEMENT REGARDING FEDERALLY SPONSORED RESEARCH

The United States Government has rights in this invention pursuant to contract no. DE-AC05-00OR22725 between the United States Department of Energy and UT-Battelle, LLC.

US Referenced Citations (75)
Number Name Date Kind
2684299 Binder Jul 1954 A
3030206 Buck, Jr. Apr 1962 A
3416916 Herchenroeder Dec 1968 A
3444058 Mellors May 1969 A
3576622 McCoy Apr 1971 A
3785877 Bailey Jan 1974 A
3811960 Perry et al. May 1974 A
3917463 Doi et al. Nov 1975 A
3985582 Bibring et al. Oct 1976 A
4102394 Botts Jul 1978 A
4194909 Ohmura et al. Mar 1980 A
4476091 Klarstrom Oct 1984 A
4512817 Duhl et al. Apr 1985 A
4652315 Igarashi et al. Mar 1987 A
4740354 Watanabe et al. Apr 1988 A
4765956 Smith et al. Aug 1988 A
4818486 Rothman et al. Apr 1989 A
4820359 Bevilacqua et al. Apr 1989 A
4877461 Smith et al. Oct 1989 A
5077006 Culling Dec 1991 A
5167732 Naik Dec 1992 A
5244515 Miglin Sep 1993 A
5330590 Raj Jul 1994 A
5529642 Sugahara et al. Jun 1996 A
5567383 Noda et al. Oct 1996 A
5585566 Welles, II et al. Dec 1996 A
5660938 Sato et al. Aug 1997 A
5718867 Nazmy et al. Feb 1998 A
5779972 Noda et al. Jul 1998 A
5788783 Coutu et al. Aug 1998 A
5888316 Erickson Mar 1999 A
5916382 Sato Jun 1999 A
5951789 Ueta et al. Sep 1999 A
6099668 Ueta et al. Aug 2000 A
6224824 Zhang et al. May 2001 B1
6344097 Limoges et al. Feb 2002 B1
6372181 Fahrmann Apr 2002 B1
6610154 Limoges et al. Aug 2003 B2
6702905 Qiao Mar 2004 B1
6797232 Speidel et al. Sep 2004 B2
6905559 O'Hara et al. Jun 2005 B2
6908518 Bouse et al. Jun 2005 B2
7011721 Harris et al. Mar 2006 B2
7038585 Hall et al. May 2006 B2
7042365 Diaz-Lopez et al. May 2006 B1
7089902 Sato et al. Aug 2006 B2
7160400 Magoshi et al. Jan 2007 B2
7450023 Muralidharan et al. Nov 2008 B2
7507306 Chen et al. Mar 2009 B2
7824606 Heazle Nov 2010 B2
7825819 Muralidharan et al. Nov 2010 B2
8147749 Reynolds Apr 2012 B2
8313591 Hirata et al. Nov 2012 B2
20030190906 Winick Oct 2003 A1
20040174260 Wagner Sep 2004 A1
20050053513 Pike Mar 2005 A1
20070152815 Meyers et al. Jul 2007 A1
20070152824 Waterhouse et al. Jul 2007 A1
20070152826 August et al. Jul 2007 A1
20070284018 Hamano Dec 2007 A1
20080001115 Qiao et al. Jan 2008 A1
20080126383 Perrin May 2008 A1
20090044884 Toschi et al. Feb 2009 A1
20090081073 Barbosa et al. Mar 2009 A1
20090081074 Barbosa et al. Mar 2009 A1
20090087338 Mitchell et al. Apr 2009 A1
20090194266 Conrad et al. Aug 2009 A1
20100008790 Reynolds Jan 2010 A1
20100116383 Cloue et al. May 2010 A1
20100303666 Bain et al. Dec 2010 A1
20100303669 Pankiw et al. Dec 2010 A1
20110236247 Osaki et al. Sep 2011 A1
20110272070 Jakobi et al. Nov 2011 A1
20120279351 Gu et al. Nov 2012 A1
20140271338 Holcomb et al. Sep 2014 A1
Foreign Referenced Citations (17)
Number Date Country
706339 Mar 1965 CA
1215255 Dec 1986 CA
2688507 Jun 2011 CA
2688647 Jun 2011 CA
100410404 Aug 2008 CN
202883034 Apr 2013 CN
1647609 Apr 2006 EP
734210 Jul 1955 GB
943141 Nov 1963 GB
5684445 Jul 1981 JP
07109539 Apr 1995 JP
2012219339 Nov 2012 JP
2479658 Apr 2013 RU
9206223 Apr 1992 WO
2008005241 Jan 2008 WO
2009145708 Dec 2009 WO
2013080684 Jun 2013 WO
Non-Patent Literature Citations (23)
Entry
Bruemmer, Stephen M. and Gary S. Was, Microstructural and Microchemical Mechanisms Controlling Intergranular Stress Corrosion Cracking in Light-Water-Reactor Systems, Journal of Nuclear Materials, 1994, pp. 348-363, , vol. 216.
Weitzel, P.S., Steam Generator for Advanced Ulta-Supercritical Power Plants 700 to 760C, Technical Paper, 2011, pp. 1-12.
Khan, T., The Development and Characterization of a High Performance Experimental Single Crystal Superalloy, pp. 145-155.
Freche, J.C., et al., Application of Powder Metallurgy to an Advanced-Temperature Nickel-Base Alloy, NASA-TN D-6560, pp. 1-22.
Ignatiev et al.: “Alloys compatibility in molten salt fluorides: Kurchatov Institute related experience”, Journal of Nuclear Materials, 441 (2013), 592-603.
Kondo et al.: “Corrosion characteristics of reduced activation ferritic steel, JLF-1 (8.92Cr-2W) in molten salts Flibe and Flinak, Fusion Engineering and Design”, 84 (2009) 1081-1085.
Kondo et al.: “High Performance Corrosion Resistance of Nickel-Based Alloys in Molten Salt FLiBe”, Fusion Science and Technology, 56, Jul. 2009, 190-194.
Delpech et al.: “MSFR: Material Issues and the Effect of Chemistry Control”, GIF Symposium, Paris France, Sep. 9-10, 2009.
Liu et al.:“Investigation on corrosion behavior of Ni-based alloys in molten fluoride salt using synchrotron radiation techniques”, Journal of Nuclear Materials, 440 (2013) 124-128.
Glazoff et al.: “Computational Thermodynamic Modeling of Hot Corrosion of Alloys Haynes 242 and HastelloyTM N For Molten Salt Service in Advanced High Temperature Reactors”, Journal of Nuclear Energy Science & Power Generation Technology, 3(3), 2014.
Materials Compatibility for High Temperature Liquid Cooled Reactor Systems (RC-1) https://neup.inl.gov/SiteAssets/FY—2017—Documents/FY17—CINR—DRAFT—WORKSCOPES.pdf.
Zheng et al: “Corrosion of 316L Stainless Steel and Hastelloy N Superalloy in Molten Eutectic LiF—NaF—KF Salt and Interaction with Graphite”, Nuclear Technology, 188(2), 2014, p. 192.
Zheng et al.: “Corrosion of 316 Stainless Steel in High Temperature Molten Li2BeF4 (FLiBe) Salt”, Journal of Nuclear Materials, vol. 416, 2015, p. 143.
Olson et al.: Impact of Corrosion Test Container Material in Molten Fluorides, Journal of Solar Energy Engineering, v. 137(6), 061007, 2015.
Zheng et al: “High Temperature Corrosion of Hastelloy N in Molten Li2BeF4 (FLiBe) Salt”, Corrosion, 71/10, 2015, p. 1257.
Barner, J.H. Von et al., “Vibrational Spectra of Fluoro and Oxofluoro Complexes of Nb(V) and Ta(V)”, Materials Science Forum vols. 73-75 (1991) pp. 279-284 © (1991) Trans Tech Publications, Switzerland doi:10.4028/www.scientific.net/MSF.73-75.279.
Devan, Jackson H., “Effect of Alloying Additions on Corrosion Behaviour of Nickel-Molybdenum Alloys in Fused Fluoride Mixtures”, ORNL-TM-2021, vol. I, J. H. DeVan; Oak Ridge National Laboratory Central Research Library Document Collection (May 1969).
Misra, Ajay K. et al., “Fluoride Salts and Container Materials for Thermal Energy Storage Applications in the Temperature Range 973 to 1400 K”, 22nd Intersociety Energy Conversion Engineering Conference cosponsored by the AIAA, ANS, ASME, SAE, IEEE, ACS, and AlChE Philadelphia, Pennsylvania, Aug. 10-14, 1987. Department of Metallurgy and Materials Science, Case Western Reserve University , Cleve.
Polyakova, L.P. et al., “Electrochemical Study of Tantalum in Fluoride and Oxofluoride Melts”, J. Electrochem. Soc., vol. 141, No. 11, Nov. 1994 The Electrochemical Society Inc., pp. 2982-2988.
Singh, Raj P. , “Processing of Ta2O5 Powders for Electronic Applications”, Journal of Electronic Materials, vol. 30, No. 12, 2001, pp. 1584-1594.
Yoder, Graydon L. et al., “An experimental test facility to support development of the fluoride-salt-cooled high-temperature reactor”, Annals of Nuclear Energy 64 (2014) 511-517.
“Advanced Sensor System for Energy Infrastructure Assurance”, Jan. 2004, Office of Energy Assurance, U.S Department of Energy, 2 pages.
ASM International, Materials Park, Ohio, Properties and Selection: Nonferrous Alloys and Special Purpose Materials: Nickel and Nickel Alloys, Oct. 1990, vol. 2, pp. 428-445.
Related Publications (1)
Number Date Country
20150197832 A1 Jul 2015 US