FIELD OF THE INVENTION
[0001] This invention relates to a method for applying thermal spray coatings to superalloys
and, more particularly, to a method for preparing a surface of the superalloy to enable
the thermal spray coating to adhere rigidly thereto.
BACKGROUND OF THE INVENTION
[0002] In general, metallic substrates which are to be coated by a thermal spray coating
process are initially roughened by a grit blast to achieve a surface roughness which
enables a good mechanical bond to be achieved. The grit blast, by its nature, leaves
a residue of grit inclusions within the substrate. The grit material may include silicon
carbide and iron particles, but in most applications is comprised of angular aluminum
particles. Silicon carbide is no longer employed for grit blasting of high temperature
superalloys due to concerns of forming low-melting phases which possibly affect stress/rupture
life. Today, substantially all grit blasting is performed using alumina particles.
The term "superalloy" includes cobalt, titanium and nickel-based alloys which exhibit
both high strength and hardness levels.
[0003] For some applications, grit inclusions present a concern. Interface specifications,
between a superalloy substrate and the coating, limit the amount of included grit.
The coatings of turbine blades for use in aircraft engines must meet highly stringent
interface inclusion limitations. Thus, the prior art has had to conform to the grit
inclusion limits, while achieving a desired level of surface roughness to assure a
rigid bond for a subsequently applied coating.
[0004] While a superalloy must exhibit a proper surface roughness to achieve a well bonded
thermal spray coating, the surface must also be clean. Thus oils, grease and surface
oxides, such as might be obtained from a prior pretreatment, are to be avoided. The
prior art has achieved clean substrates by requiring use of a wet abrasive cleaning
process which also adds fine grit inclusions to the superalloy surface. As the wet
abrasive cleaning process was followed by a dry grit blast process, the combination
added significant inclusions, i.e., up to 15% of the interface level. The presence
of alumina grit inclusions on an otherwise clean interface has been found to allow
reactions to occur during a subsequent heat treatment which result in undesirable
interface decoration.
[0005] Accordingly, it is an object of this invention to provide an improved method for
achieving a level of surface roughness of a superalloy wherein grit inclusions are
avoided.
[0006] It is a further object of this invention to provide an improved method for roughening
a surface of a superalloy by employing a high pressure liquid jet.
SUMMARY OF THE INVENTION
[0007] A liquid jet is employed to roughen the surface of a substrate so as to enable a
subsequent thermal spray coating material to adhere tightly to the surface. The substrate
is preferably a superalloy that is either nickel or cobalt based. The method initially
provides a high pressure liquid jet and moves the liquid jet across the substrate
surface at a rate so as to deliver liquid to the surface in a range of amounts of
at least approximately 0.7 kg/cm
2 to approximately 5.5 kg/cm
2. The high pressure liquid jet is preferably provided from a reservoir that is maintained
at a pressure in the range of approximately 28 ksi to 52 ksi. A preferred embodiment
employs an initial blast of a grit to the surface of the substrate to remove a smooth
finish from the substrate, prior to the application of the liquid jet. The initial
grit blast enables substantially lessened pressures and amounts of applied liquid
mass to accomplish desired ranges of surface roughening.
BRIEF DESCRIPTION OF THE DRAWINGS
[0008] Fig. 1 is a plot of metal erosion versus mass of water delivered, showing erosion
of IN-718 for reservoir-pressures of 30 ksi, 40 ksi, and 50 ksi.
[0009] Fig. 2 is a plot of metal erosion versus mass of water delivered, showing erosion
of aged IN-718 for reservoir pressures of 30 ksi, 40 ksi, and 50 ksi.
[0010] Fig. 3 is a plot of metal erosion versus mass of water delivered showing erosion
of a grit blasted IN-718 for reservoir pressures of 30 ksi, 40 ksi, and 50 ksi.
[0011] Fig. 4 is a plot of metal erosion versus water jet pressure for IN-718, showing a
comparison between a grit blast surface and a surface which has not been grit blasted.
[0012] Fig. 5 is a plot of erosion weight loss versus mass of water delivered for a variety
of superalloys from a reservoir maintained at 50 ksi.
[0013] Fig. 6 is a plot of metal erosion versus mass of water delivered for MAR-M 509 from
a reservoir maintained at 32 ksi, 40 ksi, and 52 ksi.
[0014] Fig. 7 is a plot of erosion weight loss versus mass of water delivered, showing erosion
of RENE 80 for a reservoir maintained at 40 ksi and 50 ksi.
[0015] Fig. 8 is a plot of surface roughness versus erosion weight loss for RENE 80 under
the conditions shown in the plot of Fig. 7.
[0016] Fig. 9 is a plot of erosion weight loss versus mass of water delivered for 3 steel
samples by a water jet from a reservoir maintained at 50 ksi.
[0017] Fig. 10 is a plot of threshold pressure versus hardness to achieve an initial erosion
by a water jet of IN-718, MAR-M 509 and RENE 80.
[0018] Fig. 11 is a plot of mass of water delivered versus water jet pressure to achieve
a 4.5 mg/cm
2 erosion for both cobalt-based and nickel based superalloys.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT
[0019] A high pressure waterjet is used to roughen a superalloy's surface in preparation
for a subsequent thermal spray coating. The objective is to reduce to a minimum, interface
inclusions in the superalloy surface from the roughening step. In many waterjet applications,
such as cutting of metals or ceramics, abrasive material is added to the high pressure
waterjet and dramatically enhances its cutting rate. This invention employs no abrasives
in the waterjet, only a pure liquid that has been filtered and cleaned by reverse
osmosis.
[0020] As will be apparent from the data below, it has been determined that a pure waterjet
exhibiting a requisite pressure can provide sufficient surface erosion of a superalloy
(or other metal) with little or no surface inclusions which adversely affect a later-applied
thermal spray coating. In addition to enabling surface erosion, the waterjet spray
further provides a cleaning action on the substrate surface.
[0021] The principal findings of this invention are as follows:
1. A critical minimum or threshold waterjet pressure is required to erode superalloys
and other metals. The threshold waterjet pressure varies with the hardness of the
substrate.
2. A minimum amount of water (or other liquid) must be delivered, and exceeded, for
measurable erosion to occur in the substrate. Until that amount of water has been
delivered, no measurable erosion occurs. The period before which erosion begins is
termed the "incubation period".
3. It has been found that a light grit blast pretreatment to remove the surface finish
of the substrate substantially accelerates a subsequent waterjet erosion action. The
light grit blast pretreatment eliminates the incubation period, enables lower waterjet
pressures to be employed and reduces the threshold waterjet pressure to achieve a
desired level of erosion.
[0022] The useful range of waterjet erosion of a substrate is when an adequate level of
roughness has been obtained, with a minimum of substrate removal. The roughness minimum
required for a thermal spray coating is approximately 80 microinches and in one superalloy
(i.e. IN-718) is achieved at approximately 5 mg/cm
2 removal (approximately 1/4 mil of thickness of the substrate). The roughness maximum
for a subsequent thermal spray coating is approximately 500 microinches due to self
masking and shadowing of a subsequent thermal spray coating and, thus, incomplete
coverage at the interface and reduced bond strength.
[0023] In order to achieve an adequate roughening of the surface, it has been determined
that an average thickness removal minimum is approximately 0.2 mils, which corresponds
to a removal of approximately 4.5 mg/cm
2 of a typical superalloy surface. The maximum thickness removal that can be accepted
is approximately 2 mils. This limit is based on a concern for the reduction in cross
section of a thin wall superalloy used for turbine blade applications. Such a thickness
removal corresponds to approximately 45 mg/cm
2 erosion of the substrate surface. It has further been determined that an adequate
and useful roughness for a subsequent thermal spray coating is approximately 160 microinches
and is obtained in IN-718 at 10 mg/cm
2 erosion.
[0024] To achieve a roughened superalloy surface suitable for a subsequent thermal spray
coating, the preferred ranges of roughness, erosion and thickness loss are as follows:
roughness - 50-500 micro inches;
erosion - 4.5-45 mg/cm2; and
thickness loss - 0.25-2.0 mls.
[0025] The more preferred ranges of roughness, erosion and thickness loss are as follows:
roughness - 80-200 micro inches;
erosion - 5-20 mg/cm2 and
thickness loss 0.25-1.0 mls.
[0026] The above ranges can be achieved by application of a pure waterjet that is scanned
across the surface in a raster manner. The waterjet must exhibit a pressure that is
at least above the threshold pressure for the alloy being roughened. Further, the
scan rate of the waterjet is set so that the mass of water applied per unit area is
greater than a critical delivered amount.
[0027] It has further been found that a pretreatment by a light grit blast applied to the
surface enables a more rapid surface roughening action by a subsequent waterjet application,
with lower waterjet pressures.
[0028] As will be apparent from the data below, the invention has been tested on both nickel-based
superalloys and cobalt-based superalloys which will be hereafter referred to by their
trade names: IN-718; MAR-M 509 and RENE 80. The compositions of each of the aforementioned
alloys (in weight %) is as follows:
TABLE 1
| IN-718 |
| carbon |
0.05 |
| chromium |
19 |
| aluminum |
0.5 |
| titanium |
1.0 |
| molybdenum |
3.0 |
| niobium |
5.0 |
| zirconium |
0.01 |
| boron |
0.005 |
| iron |
18 |
TABLE 2
| MAR - M 509 |
| carbon |
0.55 - 0.65 |
| chromium |
21.0 - 24.0 |
| nickel |
9.0 - 11.0 |
| tungsten |
6.5 - 7.5 |
| tantalum |
3.0 - 4.0 |
| titanium |
0.15 - 0.25 |
| zirconium |
0.40 - 0.60 |
| manganese |
0.10 max |
| silicon |
0.40 max |
| boron |
0.01 max |
| iron |
1.50 max |
| sulphur |
0.015 max |
| cobalt |
remainder |
TABLE 3
| RENE 80 |
| cobalt |
9.5 |
| chromium |
14 |
| molybdenum |
4 |
| tungsten |
4 |
| titanium |
5 |
| aluminum |
3 |
| carbon |
0.17 |
| zirconium |
0.03 |
| boron |
0.015 |
| nickel |
balance |
EXPERIMENTAL
[0029] Experimental work was accomplished employing a Flow International Model 9X Pressure
Intensifier capable of 358 MegaPascals (52 ksi) maximum water pressure. The waterjet
was defined by a 0.4 mm (0.016 inch) diameter sapphire orifice and the stream was
rastered across test substrates at various traverse speeds, but all with a common
0.76 mm (0.03 inch) offset between raster traces. The stand-off from the substrate
surface to the jet exit nozzle was 7.6 cm (3 inches) throughout, which was found to
be the distance for maximum erosion effect.
[0030] A single erosion trace had a width of approximately 1.5 mm (0.06 inches). The alloy
substrates were weighed before and after waterjet exposure as well as their thicknesses
were measured. The erosion was calculated as milligrams of mans lost, per square centimeter
of surface area. Most of the samples were round buttons, 25.4 mm in diameter and 3.2
mm thick but some were of odd coupon dimensions, cut from turbine blade roots or sheet
stock. The high pressure pump had the following water flow rates through the 0.4 mm
orifice. At 207,276 and 345 MPa (30, 40 and 50 ksi) reservoir pressures: 3.49, 3.97,
and 4.50 liters/minute.
[0031] From these flow rates and raster rate, the mass of water delivered to each specimen
was calculated in kilograms per square centimeter.
[0032] An initial survey of the effect of the high pressure jet on various alloy coupons
was performed at a 50 ksi reservoir pressure and a 30.5 cm/min. traverse rate. Based
on these results, another mating specimen was run at either a faster or slower traverse
rate, depending on whether the first erosion loss was relatively large or small. These
multipoint data sets are shown in the Figs.
[0033] The IN-718 was solution annealed for one hour at 954°C (1750°F) and had a Rockwell
B hardness of 103. The MAR-M 509 coupons were in an as - cast condition with a superficial
Rockwell C hardness of 31.0. The RENE 80 coupon were cut transversely from a directionally
solidified rod, which had been given a standard solution anneal of four hours at 1200°C
in vacuum, with a final hardness of 39.4 HRc. The original MAR - M 509 surfaces were
ground and then vibratory finished with triangular aluminum media in water, producing
an initial surface finish of 0.5 micrometers. The RENE 80 was surface ground to a
0.3 micrometer finish. The eroded surfaces were examined on a scanning electron microscope
and the roughness measured with a portable Taylor-Hobsen profilometer at a 0.76 mm
(0.03 inches) cutoff setting.
[0034] Fig. 1 is a plot for IN-718 of mass of water delivered (in kg/cm
2) versus metal eroded (mg/cm
2). Two important features of the waterjet erosion process are evident from the plot
of Fig. 1. One is that there is a minimum mass of water required to impinge on the
IN-718 substrate before there is a measurable erosion, that is, an incubation period.
Thus, at 40 ksi, substantial erosion does not occur until after 0.8 kg/cm
2 of water has been delivered across the substrate. At such time, erosion commences
and increases in exponential fashion. At 50 ksi, the incubation period terminates
at approximately 0.5 kg/cm
2.
[0035] The second feature is that there is a threshold pressure required for measurable
erosion and that 30 ksi is only slightly above that threshold. The erosion threshold
jet pressure can be determined from the initial slopes of the curves. It has been
determined that a threshold for solution annealed IN-718 is approximately 28.5 ksi(196
MPa). From the Bernoulli equation, the threshold pressure can be converted to jet
velocity, and thus the corresponding threshold velocity for IN-718 is 650 meters per
second.
[0036] In Fig. 2, similar erosion conditions were performed on an aged IN-718 coupon which
had been annealed for one hour at 1750°F and then aged, for eight hours, at 1325°F
plus an additional 10 hours at 1150°F. The aged IN-718 had a Rockwell B hardness of
115. Note that the metal erosion values were considerably less than those shown in
Fig. 1, evidencing a distinct dependence upon substrate hardness.
[0037] The experiments shown in Fig. 1 were repeated, for an IN-718 coupon which had been
subjected to a pretreatment of a light grit blast to remove the original smooth finish
of the coupon (see Fig. 3). A 240 mesh angular alumina grit was employed with a blast
head positioned 2 inches from the coupon at a 90° impingement angle. The applied grit
pressure was 35 psig. Subsequent to the grit blast pretreatment, the coupon was subjected
to a waterjet erosions at 30 ksi, 40 ksi and 50 ksi reservoir pressures. Note that
in each case, a substantial increase in metal erosion value is evident at the respective
waterjet pressures.
[0038] In Fig. 4, a direct comparison is shown between metal erosion values for a sample
which was grit blasted and then subjected to a waterjet roughening procedure versus
a portion of the same sample which was subjected to the waterjet roughening procedure,
without the initial grit blast. In the plot of Fig. 4, the amount of metal erosion
is plotted against waterjet pressure and it is to be noted that erosion commences
at a considerably lesser pressure when the sample has been grit blasted as compared
to the non-grit blasted sample.
[0039] In Fig. 5, the mass of water delivered to the substrate is plotted against erosion
weight loss for a variety of materials which have been subjected to a 50 ksi waterjet
roughening procedure. The IN-718 data discussed above (solution annealed 1hr at 1750°F)
is plotted and erosion data for an IN-718 coupon in an over-solution condition (4hrs.
at 1975°F) has been added as well as data for a sample of titanium - 6 wt. percent
aluminum - 4 wt. percent vanadium. The titanium alloy behaved somewhat like the IN-718
(1 hr./1750°F), but the IN-718 (4 hrs./1975°F) exhibited a much higher erodability
for a like mass of water delivered. As can be seen from the data plotted in Fig. 5,
there was substantial difference in the erosion weight loss achieved in the IN-718
samples, depending upon the heat treatment state. For the case of waterjet erosion
at 50 ksi, a 40 mg/cm
2 weight loss achieved a 7.5 micrometer roughness in IN-718 annealed 1 hr. at 1750°F,
but a 11.5 micrometer roughness in the IN-718 annealed 4 hrs. at 1975°F. At the same
jet pressure and mass of water delivered, the over-solution material had substantially
more erosion loss and greater roughness.
[0040] The trend of MAR-M 509 erosion as a function of mass of water delivered to the substrate
is shown in Fig. 6. The 359 MPa (52 ksi) erosion data curve increases exponentially
with increasing mass of water impingement. A similar but still exponential curve is
seen at 276 MPa (40 ksi), with both curves suggesting a threshold or incubation period
occurring at the initiation of the erosion action.
[0041] In Fig. 7, the erosion of RENE 80 is shown in a plot of erosion weight loss versus
mass of water delivered. Note that it is clearly seen that there is a threshold value
of approximately 1 kg/cm
2 before measurable erosion occurs.
[0042] The surface roughness of the eroded RENE 80 coupons is shown in Fig. 8 as a function
of erosion weight loss. The roughness rises quickly with erosion and then moves towards
a limiting value of approximately 30 micrometers at a very high eroded weight loss.
Recall that the 220 mg/cm
2 weight loss corresponds to approximately a 10.6 mil surface removal. This is substantially
more than the modest surface removal required for thermal spray preparation. However,
at a weight loss of approximately 10 mg/cm
2, it was found that a roughness of approximately 5 micrometers occurred which was
quite adequate for a subsequent thermal spray application.
[0043] In Fig. 9, the results of waterjet erosion tests on steels having hardnesses of 40,
50 and 60 Rockwell "C" are shown. Here again, it is to be noted that the erosion weight
loss is substantially dependent upon the hardness of the substrate, as well as the
applied waterjet pressure and mass of water delivered.
[0044] To demonstrate that a substrate which has been subjected to a waterjet roughening
procedure will provide a good base for a plasma spray coating, a nickel based superalloy
turbine blade was cleaned and roughened in one step using appropriate waterjet parameters
found above. The blade had a dark surface oxide originally, but it was removed completely
by the waterjet roughening procedure. The erosion weight loss of the blade was 10.7
mg/cm
2, about 0.012 mm thickness removal. The blade was then coated with an MCrAlY overlay
(where M is, nickel, cobalt or iron) by an argon shrouded plasma spray, heat treated
in a vacuum, finished and peened. An excellent bond was obtained and the interface
was absolutely clean everywhere.
[0045] The results above indicate that each tested substrate material exhibits a threshold
pressure below which surface erosion does not commence. In Fig. 10, a plot is shown
of threshold pressure versus hardness (Rockwell B) for the three principal superalloys
that were studied, IN-718; MAR-M 509 and RENE 80. Note that as the hardness increases,
the threshold pressure increases in an exponential fashion.
[0046] In Fig. 11, the mass of water delivered is plotted against waterjet pressure for
both cobalt-based superalloys and nickel-based superalloys. In each case, the mass
of water delivered was that required to achieve a 4.5 mg/cm
2 erosion of the substrate. Note that for cobalt-based superalloys, the mass of water
delivered varies from approximately 0.7 kg/cm
2 at 52 ksi to 5.5 kg/cm
2 at approximately 31.5 ksi. By contrast, the nickel based superalloys exhibit a lesser
mass of water required to achieve a similar erosion state and at lower waterjet pressures
(e.g. approximately 1.5 kg/cm
2 at 40 ksi.
[0047] In summary, the above studies indicate that threshold waterjet pressures are present
for each substrate material below which erosion will not occur. Those pressure are
shown in Table 4.
TABLE 4
| THRESHOLD PRESSURE |
| Material |
Ksi |
| MAR-M 509 |
30.6 |
| RENE - 80 |
36.2 |
| IN-718 |
28.5 |
[0048] Table 5 below denotes the critical mass of water needed to achieve the stated levels
of erosion in the variety of substrates subjected to test. Each of the entries in
Table 5 establishes, for at least a minimum erosion level of 4.5 mg/cm
2, the mass of required water at the indicated pressure. Also, there is an entry (for
all but one substrate) which indicates the mass of water required to achieve a maximum
level of erosion of 45 mg/cm
2. The entries in Table 5 which have an asterisk are interpolated values between experimentally
achieved values.
TABLE 5
| CRITICAL MASS OF H2O TO ACHIEVE STATED EROSION |
| SUBSTRATE |
EROSION (mg/cm2) |
Mass of H2O (kg/cm2) at Pressure (ksi) |
| |
|
30 |
32 |
40 |
41 |
44 |
50 |
52 |
| MAR M 509 |
4.5 |
|
5.4 |
|
2.3* |
|
|
0.7 |
| |
45 |
|
>12 |
|
12.4* |
|
|
5.0 |
| RENE 80 |
|
|
|
|
|
|
|
|
| Solution Anneal 4 hrs. (2200°F) |
4.5 |
|
|
1.6 |
|
|
0.9 |
|
| 45 |
|
|
5.4 |
|
|
2.5 |
|
| IN-718 |
|
|
|
|
|
|
|
|
| Solution Anneal 1 hr. (1750°F) |
4.5 |
>2 |
|
1.3 |
|
|
0.8 |
|
| 45 |
>>2 |
|
>2 |
|
|
2.2 |
|
| IN-718 |
|
|
|
|
|
|
|
|
| Solution Anneal 1 hr./1750°F w/ grit blast |
4.5 |
1.5 |
|
0.8 |
|
|
0.45 |
|
| 45 |
>>2 |
|
2.55* |
|
|
1.75 |
|
| IN-718 |
|
|
|
|
|
|
|
|
| Aged |
4.5 |
>>2 |
|
2.1 |
|
|
1.3 |
|
| STEELS |
|
|
|
|
|
|
|
|
| Rockwell C 40 |
4.5 |
|
|
|
|
|
1.8 |
|
| Rockwell C 40 |
45 |
|
|
|
|
|
3.6 |
|
| Rockwell C 50 |
4.5 |
|
|
|
|
|
2.0 |
|
| Rockwell C 50 |
45 |
|
|
|
|
|
5.8 |
|
| Rockwell C 60 |
4.5 |
|
|
|
|
|
4.2 |
|
| Rockwell C 60 |
45 |
|
|
|
|
|
>>12 |
|
[0049] While the above description has been based upon the use of water as the jet erosion
source, those skilled in the art will realize that other pure liquids can be appropriately
substituted. Such liquids are ethylene glycol, high density alcohols, polywater, etc.
[0050] It should be understood that the foregoing description is only illustrative of the
invention. Various alternatives and modifications can be devised by those skilled
in the art without departing from the invention. Accordingly, the present invention
is intended to embrace all such alternatives, modifications and variances which fall
within the scope of the appended claims.
1. A method for roughening a surface of a substrate, said method comprising the steps
of:
a. providing a pre-roughening by a blast of grit across the surface of the substrate;
b. providing a liquid jet of at least 28 ksi pressure; and
c. moving said liquid jet across said surface of said substrate at a rate so as to
deliver the liquid to said surface in a range on amounts between 0.7 kg/cm2 and 5.5kg/cm2.
2. The method of claim 1 wherein the following step is added:
a. depositing a layer of metallic, ceramic, or cermet material upon said surface using
a thermal spray coating device.
3. The method of claim 1, wherein the jet pressure and the amount of liquid delivered
to said surface is adjusted to roughen said surface to within a range of 50 - 500
microinches.
4. The method of claim 1, wherein the jet pressure and the amount of liquid delivered
to said surface are adjusted to erode said surface to a thickness loss not exceeding
2.0 mils.
5. The method recited in claim 1, wherein said substrate is a superalloy selected from
the group consisting of nickel based alloys, cobalt based alloys, iron based alloys,
and titanium based alloys.
6. The method of claim 1, wherein said liquid jet comprises a flow of liquid selected
from the group consisting of water, ethylene glycol, alcohols and polywater.
7. The method of Claim 2, wherein the thermal coating spray device is selected from the
group consisting of plasma spray, detonation gun, high velocity oxy-fuel, and high
velocity impact fusion.