TECHNICAL FIELD
[0001] The present invention relates to a method for producing a Ni-based heat resistant
superalloy.
BACKGROUND ART
[0002] Turbine operation at high temperatures is considered to be effective improving the
efficiency of aircraft engines and power generation efficiency of gas turbines. To
that end, it is important to increase the service temperature of each turbine member.
In particular, for members that require a service temperature of 600°C or higher,
a y' (gamma prime) phase-precipitation strengthening Ni-based heat resistant superalloy
is often used. The γ' phase is an intermetallic compound of L1
2 structure represented by Ni
3Al, and it is known that dissolving elements such as Ti, Nb, and Ta in the y' phase
further enhances the effect of precipitation strengthening. The y' phase-precipitation
strengthening Ni-based heat resistant superalloy is mainly composed of two phases:
a matrix γ phase and a precipitation phase γ' phase, and when the amount of Ti or
Nb is increased, an intermetallic compound such as an eta phase (such as Ni
3Ti) or a delta phase (such as Ni
3Nb) may be precipitated as the third phase. Furthermore, C and B are often added mainly
to strengthen the grain boundary of the matrix, and trace amounts of carbides and
borides may be crystallized or precipitated.
[0003] As described above, increasing the amount of Al, Ti, Nb, and Ta that form and strengthen
the y' phase is effective to enhance the high temperature strength of the Ni-based
heat resistant superalloy. This increases the amount of precipitation of the y' phase
and strengthens the y' phase itself. Examples of the high-strength Ni-based heat resistant
superalloys include Udimet 720 Li (Udimet is a registered trademark of Special Metals).
[0004] Although the Ni-based heat resistant superalloy containing a large amount of Ti,
Nb, and Ta is high in strength, microsegregation may easily remain even after hot
working, and it is difficult to obtain a homogeneous microstructure. The main reason
for the microsegregation is considered to be that the added elements in the alloy
are distributed unevenly in the solid or liquid phase during the precipitation process.
In particular, since the elements that contribute to the increase in precipitation
amount and strengthening of the γ' phase, such as Ti, Nb, and Ta, easily concentrate
at the liquid phase side during the precipitation processing of the ingot, microsegregation
occurs in inside the ingot after the precipitation is completed. This microsegregation
further accelerates as the precipitation rate is slower; thus, the larger the size
of the ingot, the more prominent is the microsegregation. To reduce this microsegregation,
a heat treatment step called homogenization treatment is generally introduced as a
next step. The homogenization treatment is often applied to the ingot, and is sometimes
also applied to a billet as an intermediate step in hot working.
[0005] The homogenization treatment is often performed at a temperature at or above the
solvus temperature and below the melting point of the second phase such as the γ'
phase. However, the appropriate conditions for the homogenization treatment, such
as the required heating temperature, holding time, and cooling rate, are not necessarily
determined because they vary greatly depending on not only the chemical composition,
but also on the solidification rate during ingot production. In the Ni-based heat
resistant superalloy with the large amount of y' precipitation, the y' phase is precipitated
during the cooling process after the homogenization treatment. Thus, the cooling rate
has a great impact on subsequent hot workability. The faster the cooling after the
homogenization treatment, the finer the y' phase precipitation. However, when hot
working is performed in this state, the movement of the displacement is easily inhibited
by the fine y' phase. As a result, the deformation resistance of the workpiece is
significantly higher and recrystallization becomes difficult, thus hot cracking may
easily occur. As a means of solving this, it is possible to coarsen the γ' phase by
slowing the cooling rate after heating, and to improve the hot workability, for example,
as disclosed in Patent Document 1.
[0006] Regarding the Ni-based heat resistant superalloy with a large amount of γ' precipitation
after the homogenization treatment, for example, Udimet 720 Li, it is possible to
obtain a uniform and fine microstructure by performing hot working in the two-phase
domain of the γ phase and the y' phase, and causing recrystallization while acting
on the γ' phase that is not dissolved as pinning grains of the γ phase grain boundary.
However, the uniformity of the microstructure after this hot working is strongly affected
by the γ' phase distribution which acts as pinning grains. This is because, the more
uneven the y' phase distribution, the coarser the grains of the γ phase in the region
having greater distances between the y' phase grains, while the finer grains in the
region having smaller distances therebetween. Thus, it is necessary to uniformly disperse
the y' phase grains to obtain a uniform microstructure after hot working. When the
microstructure is non-uniform, practical undesirable events may occur, for example,
fatigue failure is likely to occur due to partially coarsened grains. Thus, the grain
distribution in the microstructure is desirably as uniform as possible.
[0007] When the Ni-based heat resistant superalloy is cooled, γ' phase is generally precipitated
in a spherical or cubic shape in the grains. It is known, however, that when the Ni-based
heat resistant superalloy with a large amount of γ' precipitation is heated to around
the solvus temperature of the y' phase or higher, and is then cooled at a slow cooling
rate, a fan-shaped y' phase (also called a fan-type γ' phase) is precipitated. This
fan-shaped y' phase is mainly precipitated from the grain boundary and grows with
the movement of the grain boundary. The order of precipitation during cooling is usually
that the fan-shaped y' phase is precipitated first, and then the spherical or cubic
intragranular y' phase is precipitated. Although the temperature range in which the
fan-shaped y' phase is precipitated is not uniformly determined, the precipitation
is particularly significant in the temperature range of from a y' phase solvus temperature
of the respective alloy to about the y' phase solvus temperature minus 50°C. Thus,
the slower the cooling rate is in this temperature range, the larger the precipitation
region of the fan-shaped y' phase, and the smaller the precipitation region of the
intragranular y' phase. This fan-shaped y' phase is coarse compared to the γ' phase
precipitated in the grain and has an extended shape with a large aspect ratio. In
other words, it can be said that the fan-shaped y' phase is a y' phase that is precipitated
with a non-uniform distribution. However, as described above, the uniform size of
the y' phase is better for obtaining a uniform microstructure after hot working in
the Ni-based heat resistant superalloy with a large amount of y' precipitation. If
a large amount of fan-shaped γ'phase is precipitated during cooling after the homogenization
treatment, it becomes difficult to obtain a uniform microstructure after hot working.
REFERENCE DOCUMENT LIST
PATENT DOCUMENT
SUMMARY OF THE INVENTION
PROBLEM TO BE SOLVED BY THE INVENTION
[0009] When a Ni-based heat resistant superalloy with a large amount of γ' precipitation
is subjected to a heating and cooling process that are a homogenization treatment,
a large amount of fan-shaped y' phase is precipitated during the cooling. This fan-shaped
y' phase is mainly precipitated from the grain boundary, and it is characterized by
being coarse compared to the y' phase precipitated in the grain, having a large aspect
ratio, and having a non-uniform distribution. The Ni-based heat resistant superalloy
with a large amount of γ' precipitation, such as Udimet 720 Li, can have a uniform
and fine microstructure by performing hot working in the two-phase domain of the γ
phase and the y' phase, and causing recrystallization while acting non-solid solution
y' phase as pinning grains of the γ phase grain boundary. However, if the fan-shaped
y' phase precipitation region described above extends widely after the homogenization
treatment, the size and distribution of the y' phase as the pinning grains become
uneven; thus, the size of the recrystallized grain generated during the subsequent
hot working process also becomes uneven, and the resulting difficulty in obtaining
a uniform microstructure is a problem.
[0010] Considering this, it is an object of the present invention to provide a method for
reducing the precipitation region of the fan-shaped y' phase in the homogenization
treatment of the Ni-based heat resistant superalloy with a large amount of γ'precipitation.
MEANS FOR SOLVING THE PROBLEM
[0011] That is, the present invention is a method for producing a Ni-based heat resistant
superalloy, in which the Ni-based heat resistant superalloy has a composition consisting
of, in % by mass, C: 0.001 to 0.100%, Al: 1.0 to 5.0%, Ti: 3.5 to 7.0%, Cr: 8 to 20%,
Co: 0 to 40%, Mo: 0 to 7.0%, W: 0 to 5.0%, Ta: 0 to 6.0%, Nb: 0 to 6.0%, B: 0.001
to 0.080%, Zr: 0 to 0.100%, Mg: 0 to 0.05%, Fe: 0 to 5.0%, and the balance of Ni with
inevitable impurities, and has a solvus temperature of a y' phase of 1080°C or higher,
the method comprising at least a step of heat-treating a material having the composition,
wherein the heat-treating step includes a heating step in which heating is performed
in a temperature range of 1170°C to 1280°C for 45 hours or more, and a cooling step
in which an average cooling rate in a temperature range from the solvus temperature
of the y' phase to the solvus temperature of the y' phase minus 50°C satisfies [average
cooling rate (°C/h)] ≥ 10 and [average cooling rate (°C/h)] ≥ 200 - 2.0 × [holding
time (h)].
[0012] The heating in the heating step is preferably performed for 45 hours or more and
300 hours or less. Alternatively, the average cooling rate is preferably 800 ≥ [average
cooling rate (°C/h)] ≥ 10. Alternatively, and preferably, the heating in the heating
step is performed for 60 hours or more, and the average cooling rate is 100 ≥ [average
cooling rate (°C/h)] ≥ 10.
EFFECTS OF THE INVENTION
[0013] According to the present invention, it is possible to efficiently reduce the precipitation
region of the fan-shaped y' phase.
BRIEF DESCRIPTION OF THE DRAWINGS
[0014]
[FIG. 1] These are diagrams showing metal microstructures of the Ni-based heat resistant
superalloys produced in Examples.
[FIG. 2] These are diagrams showing metal microstructures of the Ni-based heat resistant
superalloys produced in Examples.
[FIG. 3] These are diagrams showing metal microstructures of the Ni-based heat resistant
superalloys produced in Examples.
[FIG. 4] These are diagrams showing metal microstructures of the Ni-based heat resistant
superalloys produced in Examples.
[FIG. 5] These are diagrams showing metal microstructures of the Ni-based heat resistant
superalloys produced in Examples.
MODE FOR CARRYING OUT THE INVENTION
[0015] The reasons of limiting the ranges of the alloy components defined in the present
invention are described below. The component values below are in % by mass.
< C: 0.001-0.100% >
[0016] C has an effect of increasing the strength of the grain boundary, and thus, the addition
of 0.001% or more C is required. If C is contained in excess, a coarse carbide is
formed and becomes deleterious, thus the upper limit is 0.100%. The range of C is
preferably 0.005% or more, and is more preferably 0.01% or more. The range of C is
also preferably 0.06% or less, and is more preferably 0.03% or less.
< Al: 1.0-5.0% >
[0017] Al is an essential element to form a γ' phase that is a strengthening phase, and
it improves the high temperature strength. The present invention is directed to alloys
with a large amount of y' phase precipitation, and thus, the addition of at least
1.0% Al is required. If Al is contained in excess, the solvus temperature of the y'
phase is excessively increased, and thus, the upper limit is 5.0%. The range of Al
is preferably 1.5% or more, and is more preferably 1.8% or more. The range of Al is
also preferably 4.0% or less, and is more preferably 3.0% or less.
< Ti: 3.5-7.0% >
[0018] Ti is an element that is replaced by the Al site of the y' phase and increases the
strength of the y' phase by solid-solution strengthening, and it also increases the
precipitation amount of the y' phase. In the present invention, the addition of at
least 3.5% Ti is required. If Ti is added in excess, however, the y' phase becomes
unstable and the eta phase is excessively precipitated, and thus, the upper limit
is 7.0%. The range of Ti is preferably 4.6% or more, and is more preferably 5.8% or
more. The range of Ti is also preferably 6.8% or less, and is more preferably 6.6%
or less.
< Cr: 8-20% >
[0019] Cr is an element that improves oxidation resistance and corrosion resistance. The
lack of Cr amount leads to cracking due to oxidation, thus 8% or more Cr is required.
If Cr is contained in excess, a brittle phase such as the sigma phase is formed, and
thus, the upper limit is 20%. The range of Cr is preferably 10% or more, and is more
preferably 12% or more. The range of Cr is also preferably 17% or less, and is more
preferably 15% or less.
< Co: 0-40% >
[0020] Co contributes to the stability of the y' phase, and thus, Co may be added as needed.
If Co is added in excess, however, a brittle phase such as the sigma phase tends to
be precipitated, and thus, the upper limit is 40%. The range of Co is preferably 35%
or less, is more preferably 30% or less, and is further preferably 28% or less. When
Co is added, the range of Co is preferably 5% or more, is more preferably 15% or more,
and is further preferably 20% or more.
< Mo: 0-7.0% >
[0021] Mo contributes to the solid-solution strengthening of the matrix and has an effect
of improving the high temperature strength and creep deformation resistance, and thus,
Mo may be added as needed. If Mo is added in excess, however, the melting point is
excessively reduced, and thus, the upper limit is 7.0%. The range of Mo is preferably
5.0% or less, is more preferably 3.5% or less, and is further preferably 3.0% or less.
When Mo is added, the range of Mo is preferably 0.5% or more, is more preferably 1.0%
or more, and is further preferably 2.0% or more.
< W: 0-5.0% >
[0022] W, like Mo, is an element that contributes to the solid-solution strengthening of
the matrix, and thus, W may be added as needed. However, since W is a heavy element,
diffusion in the alloy is less likely to occur, and thus, the upper limit is 5.0%.
The range of W is preferably 4.0% or less, is more preferably 2.5% or less, and is
further preferably 1.6% or less. When W is added, the range of W is preferably 0.5%
or more, is more preferably 0.8% or more, and is further preferably 1.0% or more.
< Ta: 0-6.0% >
[0023] Ta, like Ti, is an element that is replaced by the Al site of the y' phase to solid-solution
strengthen the y' phase, and it increases the high temperature strength. Thus, Ta
may be added as needed to obtain high-strength alloys. However, excessive addition
of Ta makes the y' phase unstable and causes formation of a large amount of the eta
phase and the delta phase, and thus, the upper limit is 6.0%. The range of Ta is preferably
5.0% or less, is more preferably 4.0% or less, and is further preferably 3.0% or less.
When Ta is added, the range of Ta is preferably 0.5% or more, is more preferably 1.0%
or more, and is further preferably 1.5% or more.
< Nb: 0-6.0% >
[0024] Nb, like Ti and Ta, is an element that is replaced by the Al site of the y' phase
to solid-solution strengthen the y' phase, and it increases the high temperature strength.
Thus, Nb may be added as needed to obtain high-strength alloys. However, excessive
addition of Nb makes the γ'phase unstable and causes formation of a large amount of
the eta phase and the delta phase, and thus, the upper limit is 6.0%. The range of
Nb is preferably 5.0% or less, is more preferably 4.0% or less, and is further preferably
3.0% or less. When Nb is added, the range of Nb is preferably 0.5% or more, is more
preferably 1.0% or more, and is further preferably 1.5% or more.
< B: 0.001-0.080% >
[0025] B is an important element for improving the grain boundary strength and improving
the creep strength and high temperature ductility, and thus, the addition of 0.001%
or more of B is required. If B is added in excess, however, the melting point is excessively
reduced, and thus, the upper limit is 0.080%. The range of B is preferably 0.003%
or more, is more preferably 0.006% or more, and is further preferably 0.010% or more.
The range of B is also preferably 0.060% or less, is more preferably 0.040% or less,
and is further preferably 0.030% or less.
< Zr: 0-0.100% >
[0026] Zr is believed to have an effect of improving the grain boundary strength, like B,
but Zr is not necessarily required. Zr, like B, the addition in excess causes melting
point reduction, and thus, the upper limit is 0.100%. The range of Zr is preferably
0.080% or less, is more preferably 0.060% or less, and is further preferably 0.050%
or less. When Zr is added, the range of Zr is preferably 0.005% or more, is more preferably
0.007% or more, and is further preferably 0.010% or more.
< Mg: 0-0.05% >
[0027] Mg has an effect of improving the grain boundary strength by fixing S, an inevitable
impurity causing grain boundary embrittlement, as a sulfide, and thus, Mg may be added
as needed. However, if the amount of Mg added is increased, the excess Mg forms harmful
intermetallic compounds, and thus, the upper limit is 0.05%. The range of Mg is preferably
0.01% or less, is more preferably 0.005% or less, and is further preferably 0.001%
or less. When Mg is added, the range of Mg is preferably 0.0003% or more, and is more
preferably 0.0005% or more.
< Fe: 0-5.0% >
[0028] Fe is an inexpensive element, and it is possible to reduce the raw material cost
of hot workpieces by replacing some of the Ni with Fe. Thus, Fe may be included as
needed. However, the excessive addition of Fe promotes the precipitation of the sigma
phase, and thus, the upper limit is 5.0%. The range of Fe is preferably 4.0% or less,
is more preferably 1.5% or less, and is further preferably 1.0% or less. When Fe is
added, the range of Fe is preferably 0.05% or more, is more preferably 0.1% or more,
and is further preferably 0.3% or more.
< Ni: Balance >
[0029] The balance is composed of Ni and inevitable impurities. Here, examples of the inevitable
impurity elements include P, S, O, N, Pb, and As, but the total amount of these elements
preferably does not exceed 0.05%.
[0030] The reasons of limiting the solvus temperature of the y' phase defined in the present
invention are described below.
< Solvus temperature of y' phase >
[0031] The γ' phase solvus temperature of the Ni-based heat resistant superalloy targeted
by the present invention is 1080°C or higher. This is because the growth rate of the
fan-shaped y' phase is remarkable in the high temperature range. In alloys having
a γ' phase solvus temperature of less than 1080°C, a microstructure with a small precipitation
region of the fan-shaped y' phase can be obtained without using the present invention.
[0032] Next, the reasons for limiting the heating temperature and the holding time during
the homogenization treatment in the heat treatment step according to the present invention
are described below.
< Temperature during homogenization treatment >
[0033] The heating temperature during the homogenization treatment defined in the present
invention is required to be in the temperature range of 1170°C to 1280°C. If the temperature
is lower than 1170°C, diffusion in the Ni-based heat resistant superalloy is insufficient
and the effect of the homogenization treatment cannot be obtained. On the other hand,
if the temperature exceeds 1280°C, the local melting in the Ni-based heat resistant
superalloy becomes significant, and thus, the effect of the homogenization treatment
also cannot be fully obtained. Note that the heating temperature during the homogenization
treatment can also be said to be a temperature that exceeds the solvus temperature
of the γ' phase.
< Holding time during homogenization treatment >
[0034] The holding time during the homogenization treatment defined in the present invention
is the total holding time during heating in the temperature range of 1170°C to 1280°C,
which is the heating temperature described above. Accordingly, the heating time in
the temperature range of less than 1170°C is not included. To obtain the effect of
the present invention, it is necessary to heat and maintain in a temperature range
in which sufficient diffusion occurs in the Ni-based heat resistant superalloy. However,
preliminary heating treatment in a temperature range less than 1170°C may be applied
as necessary, because it is effective to avoid local melting in the precipitation
structure.
[0035] The holding time during the homogenization treatment defined in the present invention
is required to be 45 hours or more. The holding time is preferably 60 hours or more,
and is more preferably 85 hours or more. This heating and holding need not be a continuous
heating, and it may be in steps. For example, a total of two homogenization treatments
may be performed on an ingot. Alternatively, for example, a single homogenization
treatment may be performed on an ingot, then the ingot may be subjected to a certain
hot working to form a billet, and the billet may be subjected to a homogenization
treatment again. The reason for defining the holding time of heating is from both
the viewpoints of reducing microsegregation and of reducing the fan-shaped y' phase
precipitation region. The Ni-based heat resistant superalloy targeted by the present
invention is prone to leave micro segregation and also to precipitate the fan-shaped
y' phase because a large amount of added elements such as Ti is present. However,
it is possible to reduce both of these at the same time by setting the holding time
to a specified value or more. The reasons of enabling reducing not only the microsegregation,
but also the fan-shaped y' phase precipitation, can be considered, although the present
invention is not limited thereto, as follows. When the holding time during the homogenization
treatment is long, micro segregation is reduced, and the concentration gradient of
solute elements such as Al, Ti, Nb, and Ta is reduced. The lower the concentration
gradient of these elements, the more uniform is the solvus temperature of the local
γ' phase in the microstructure. Then, the region in which the solute element is concentrated,
that is, the region in which the starting temperature of the fan-shaped y' phase precipitation
is locally high is reduced during cooling from a temperature higher than the solvus
temperature of the y' phase. Accordingly, it is possible to delay precipitation and
growth. The longer the holding time during the homogenization treatment, the greater
the effect, and thus, the upper limit of the holding time is not specified. However,
from the viewpoint of working time, the holding time is preferably 300 hours or less.
< Cooling rate after homogenization treatment >
[0036] The cooling rate after the homogenization treatment defined in the present invention
is the average cooling rate in the temperature range of "50°C" from the y' phase solvus
temperature to the γ'phase solvus temperature minus 50°C. Increasing the cooling rate
in this temperature range enables reducing the precipitation region of the fan-shaped
γ' phase. The average cooling rate defined in the present invention is required to
satisfy [average cooling rate (°C/h)] ≥ 200 - 2.0 × [holding time (h)]. This means
that the longer the holding time described above, the slower the acceptable cooling
rate. The present invention is not limited by the weight of the material to be applied,
but it is particularly effective in large ingots that weigh several hundred kg or
more. Large ingots tend to have significant microsegregation due to slow precipitation
rates, and tend to have fan-shaped γ' phase precipitation during cooling after the
homogenization treatment. However, if the cooling rate after the homogenization treatment
is excessively increased to avoid the fan-shaped y' phase precipitation, the surface
temperature of the ingot preferentially decreases, resulting in easily causing cooling
cracking. This cracking sensitivity increases as the ingot becomes larger, and thus,
specifying the cooling rate after the homogenization treatment alone is not sufficient
for practical purposes. In the present invention, since the minimum required average
cooling rate is determined from the holding time, an efficient homogenization treatment
is possible in that the precipitation of the fan-shaped y' phase can be reduced while
avoiding the cooling cracking. The average cooling rate is required to satisfy at
least 10°C/h or more, in addition to the inequality expression described above. The
average cooling rate is preferably 25°C/h or more, and more preferably 40°C/h or more.
The upper limit of the cooling rate is not specified, but from the viewpoint of cooling
cracking and subsequent hot workability, it is preferably 800°C/h or less, and is
more preferably 500°C/h or less. It is possible to reduce the precipitation region
of the fan-shaped y' phase even when the average cooling rate is reduced to 100°C/h
or less by ensuring a long holding time (for example, ensuring 60 hours or more).
[0037] It should be noted that the average cooling rate is preferably maintained beyond
the temperature range of "50°C", which is from the y' phase solvus temperature to
the y' phase solvus temperature minus 50°C, even to 900.
EXAMPLES
[0038] To confirm the effect of the present invention, the homogenization treatment was
tested by the following procedure. First, an electrode of the Ni-based heat resistant
superalloy was prepared in a vacuum induction furnace (VIM), then the electrode was
refined and dissolved by electroslag remelting (ESR), and then it was further refined
and dissolved by vacuum arc remelting (VAR) to yield a VAR ingot of the Ni-based heat
resistant superalloy with a weight of about 1.0 to 1.5 tons and a diameter of about
450 mm. The chemical composition of this material is shown in Table 1. The γ' phase
solvus temperature of the alloy having this chemical composition is approximately
1165°C.
[Table 1]
| % by mass |
| |
Ni |
Cr |
Co |
Fe |
W |
Mo |
Al |
Ti |
C |
B |
Zr |
Mg |
| Present invention |
Bal. |
13.4 |
24.3 |
0.6 |
1.2 |
2.8 |
2.3 |
6.3 |
0.014 |
0.015 |
0.03 |
0.0007 |
| *The balance is composed of Ni and inevitable impurities. |
[0039] Next, the top side of the VAR ingot was cut, and a small piece of material of about
10 mm × 15 mm × 20 mm was cut from a location 1/4 the diameter from the surface. The
top side of the VAR ingot was used because the microsegregation of this part was remarkable,
and this part can be said to be a suitable material for confirming the effect of the
present invention. The cut-out small piece of material was sealed in a stainless steel
can, and it was then subjected to a homogenization treatment shown in Table 2. The
homogenization treatment was performed with an electric furnace. In the homogenization
treatment, the small piece of material was first preheated at a predetermined temperature
for a predetermined holding time, was then heated to a heating temperature of the
homogenization treatment, and was then retained at this heating temperature for a
predetermined time. In the subsequent cooling step, the cooling rate described in
Table 2 is the average cooling rate in the "temperature range from 1165°C to 1115°C".
Table 2 also shows the value A calculated from 200 - 2.0 × [holding time (h)]. No.
4 to No. 11 in the table satisfy the holding time and the average cooling rate defined
in the present invention. The cooling rate after this homogenization treatment was
maintained at least until 900°C, and then the small piece of material was continuously
cooled to room temperature in the furnace at the corresponding cooling rate as it
set, or it was taken out of the furnace after confirming that the temperature was
900°C or lower and cooled to room temperature.
[Table 2]
| No. |
Preliminary heating |
Homogenization treatment |
Notes |
| Temperature |
Holding time |
Heating rate |
Temperature |
Holding time |
Cooling rate |
Value A |
| °C |
h |
°C/h |
°C |
h |
°C/h |
| 1 |
1100 |
1 |
60 |
1200 |
35 |
60 |
130 |
Comparative example |
| 2 |
1100 |
1 |
60 |
1200 |
65 |
25 |
70 |
Comparative example |
| 3 |
1100 |
1 |
60 |
1200 |
80 |
25 |
40 |
Comparative example |
| 4 |
1100 |
1 |
60 |
1200 |
48 |
200 |
104 |
Present invention |
| 5 |
1100 |
1 |
60 |
1200 |
65 |
100 |
70 |
Present invention |
| 6 |
1100 |
1 |
60 |
1200 |
120 |
60 |
-40 |
Present invention |
| 7 |
1100 |
1 |
60 |
1200 |
200 |
60 |
-200 |
Present invention |
| 8 |
1100 |
1 |
60 |
1200 |
300 |
25 |
-400 |
Present invention |
| 9 |
1100 |
1 |
60 |
1200 |
80 |
80 |
40 |
Present invention |
| 10 |
1143 |
30 |
20 |
1200 |
96 |
60 |
8 |
Present invention |
| 11 |
1143 |
30 |
5 |
1200 |
96 |
60 |
8 |
Present invention |
[0040] The small piece of material after the homogenization treatment was cut so that the
longitudinal direction of the VAR ingot formed the observation surface. The observation
surface of the small piece of material was subjected to mirror polishing, followed
by electrolytic etching in 10% aqueous oxalic acid solution to facilitate the observation
of the y' phase. The observation of the microstructure was performed with an optical
microscope. The photographs of the microstructures of No. 1 to No. 11 in Table 2 are
shown in FIGs. 1(A), 1(B), 1(C), 2(D), 2(E), 3(F), 3(G), 4(H), 4(I), 5(J), and 5(K),
respectively, in this order.
[0041] First, as shown in FIGs. 1(A), 1(B) and 1(C), it was found that the microstructures
of No. 1, No. 2, and No. 3 had a wide range of the fan-shaped y' phase precipitated
on or near the grain boundary. These homogenization treatment conditions are beyond
the scope of the present invention since the value A was greater than the cooling
rate, as shown in Table 2.
[0042] Next, No. 6 and No. 7, which had the same cooling rate of 60°C/h as No. 1 and an
increased holding time of 120 hours and 200 hours, respectively, were confirmed to
have significantly reduced precipitation regions of the fan-shaped y' phase compared
to No. 1, as shown in FIGs. 3(F) and 3(G). In addition, No. 8, which had the same
cooling rate of 25°C/h as No. 2 and No. 3 and an increased holding time of 300 hours,
was also confirmed to have a significantly reduced precipitation region of the fan-shaped
y' phase, as shown in FIG. 4(H). From the above, it was confirmed that the homogenization
treatment with long holding time as proposed by the present invention has the effect
of greatly reducing the precipitation region of the fan-shaped y' phase.
[0043] Then, No. 5, which had the same holding time as No. 2 and a cooling rate of 100°C/h,
was confirmed to have a small precipitation region of the fan-shaped y' phase, as
shown in FIG. 2(E). In addition, No. 9, which had the same holding time as No. 3 and
a cooling rate of 80°C/h, was also confirmed to have a small precipitation region
of the fan-shaped y' phase, as shown in FIG. 4(I). Furthermore, No. 4, which has the
shortest holding time of 48 hours but the fastest cooling rate of 200°C/h in Table
2, was confirmed to have a small precipitation region of the fan-shaped y' phase,
as shown in FIG. 2(D). From the above, it was confirmed that increasing the cooling
rate after the homogenization treatment as proposed by the present invention has the
effect of greatly reducing the precipitation region of the fan-shaped y' phase.
[0044] In addition, the microstructures of No. 10 and No. 11, which had the different preheating
temperature and subsequent heating rate, were also confirmed to have a small precipitation
region of the fan-shaped y' phase, as shown in FIGs. 5(J) and 5(K).