CA2025302A1 - Reinforced microlaminted metal-matrix-composite structure - Google Patents
Reinforced microlaminted metal-matrix-composite structureInfo
- Publication number
- CA2025302A1 CA2025302A1 CA002025302A CA2025302A CA2025302A1 CA 2025302 A1 CA2025302 A1 CA 2025302A1 CA 002025302 A CA002025302 A CA 002025302A CA 2025302 A CA2025302 A CA 2025302A CA 2025302 A1 CA2025302 A1 CA 2025302A1
- Authority
- CA
- Canada
- Prior art keywords
- metal
- materials
- guns
- microlaminated
- plasma
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Abandoned
Links
- 239000011156 metal matrix composite Substances 0.000 title abstract description 5
- 229910052751 metal Inorganic materials 0.000 claims abstract description 38
- 239000002184 metal Substances 0.000 claims abstract description 38
- 239000007921 spray Substances 0.000 claims abstract description 32
- 239000000463 material Substances 0.000 claims description 49
- 238000000034 method Methods 0.000 claims description 21
- 239000000919 ceramic Substances 0.000 claims description 19
- 150000002739 metals Chemical class 0.000 claims description 8
- 230000003014 reinforcing effect Effects 0.000 claims description 3
- 230000002787 reinforcement Effects 0.000 claims description 2
- 239000011229 interlayer Substances 0.000 claims 2
- 239000010410 layer Substances 0.000 claims 1
- 229910010293 ceramic material Inorganic materials 0.000 abstract description 4
- 239000002131 composite material Substances 0.000 description 29
- 239000000843 powder Substances 0.000 description 27
- 239000000758 substrate Substances 0.000 description 25
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 23
- 229910052593 corundum Inorganic materials 0.000 description 22
- 229910001845 yogo sapphire Inorganic materials 0.000 description 22
- 238000000151 deposition Methods 0.000 description 21
- 230000008021 deposition Effects 0.000 description 20
- 239000000203 mixture Substances 0.000 description 18
- 238000000576 coating method Methods 0.000 description 17
- 229910001374 Invar Inorganic materials 0.000 description 13
- 238000012360 testing method Methods 0.000 description 13
- TWNQGVIAIRXVLR-UHFFFAOYSA-N oxo(oxoalumanyloxy)alumane Chemical compound O=[Al]O[Al]=O TWNQGVIAIRXVLR-UHFFFAOYSA-N 0.000 description 10
- 230000015572 biosynthetic process Effects 0.000 description 9
- PXHVJJICTQNCMI-UHFFFAOYSA-N Nickel Chemical compound [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 description 8
- 238000010438 heat treatment Methods 0.000 description 8
- 239000002245 particle Substances 0.000 description 8
- 238000012545 processing Methods 0.000 description 8
- 229910052802 copper Inorganic materials 0.000 description 7
- 239000010949 copper Substances 0.000 description 7
- 239000007789 gas Substances 0.000 description 7
- 230000001965 increasing effect Effects 0.000 description 7
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 6
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 6
- MCMNRKCIXSYSNV-UHFFFAOYSA-N Zirconium dioxide Chemical compound O=[Zr]=O MCMNRKCIXSYSNV-UHFFFAOYSA-N 0.000 description 6
- 230000008901 benefit Effects 0.000 description 6
- 239000011248 coating agent Substances 0.000 description 6
- 239000004615 ingredient Substances 0.000 description 6
- 238000000926 separation method Methods 0.000 description 6
- 238000005382 thermal cycling Methods 0.000 description 6
- 229910045601 alloy Inorganic materials 0.000 description 5
- 239000000956 alloy Substances 0.000 description 5
- 230000032798 delamination Effects 0.000 description 5
- 229910052759 nickel Inorganic materials 0.000 description 5
- 230000004888 barrier function Effects 0.000 description 4
- 230000000694 effects Effects 0.000 description 4
- 230000003647 oxidation Effects 0.000 description 4
- 238000007254 oxidation reaction Methods 0.000 description 4
- 239000012720 thermal barrier coating Substances 0.000 description 4
- 229910002065 alloy metal Inorganic materials 0.000 description 3
- 229910052786 argon Inorganic materials 0.000 description 3
- -1 chromium carbides Chemical class 0.000 description 3
- 230000008018 melting Effects 0.000 description 3
- 238000002844 melting Methods 0.000 description 3
- 229910052804 chromium Inorganic materials 0.000 description 2
- 239000011651 chromium Substances 0.000 description 2
- 230000003247 decreasing effect Effects 0.000 description 2
- 238000009826 distribution Methods 0.000 description 2
- 238000002474 experimental method Methods 0.000 description 2
- 238000010191 image analysis Methods 0.000 description 2
- 230000001976 improved effect Effects 0.000 description 2
- 238000011835 investigation Methods 0.000 description 2
- 238000004377 microelectronic Methods 0.000 description 2
- 238000001000 micrograph Methods 0.000 description 2
- 238000002360 preparation method Methods 0.000 description 2
- 230000008569 process Effects 0.000 description 2
- 229910000601 superalloy Inorganic materials 0.000 description 2
- KUAZQDVKQLNFPE-UHFFFAOYSA-N thiram Chemical compound CN(C)C(=S)SSC(=S)N(C)C KUAZQDVKQLNFPE-UHFFFAOYSA-N 0.000 description 2
- 238000012546 transfer Methods 0.000 description 2
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 1
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 1
- VYZAMTAEIAYCRO-UHFFFAOYSA-N Chromium Chemical compound [Cr] VYZAMTAEIAYCRO-UHFFFAOYSA-N 0.000 description 1
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical compound [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 description 1
- ZOKXTWBITQBERF-UHFFFAOYSA-N Molybdenum Chemical compound [Mo] ZOKXTWBITQBERF-UHFFFAOYSA-N 0.000 description 1
- 229910000831 Steel Inorganic materials 0.000 description 1
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 description 1
- QCWXUUIWCKQGHC-UHFFFAOYSA-N Zirconium Chemical compound [Zr] QCWXUUIWCKQGHC-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 238000013459 approach Methods 0.000 description 1
- 230000009286 beneficial effect Effects 0.000 description 1
- 229910052796 boron Inorganic materials 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 239000012159 carrier gas Substances 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 239000008199 coating composition Substances 0.000 description 1
- 239000010941 cobalt Substances 0.000 description 1
- 229910017052 cobalt Inorganic materials 0.000 description 1
- GUTLYIVDDKVIGB-UHFFFAOYSA-N cobalt atom Chemical compound [Co] GUTLYIVDDKVIGB-UHFFFAOYSA-N 0.000 description 1
- 230000000052 comparative effect Effects 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 150000001879 copper Chemical class 0.000 description 1
- 238000005520 cutting process Methods 0.000 description 1
- 125000004122 cyclic group Chemical group 0.000 description 1
- 230000001351 cycling effect Effects 0.000 description 1
- 238000000354 decomposition reaction Methods 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 238000011156 evaluation Methods 0.000 description 1
- 230000002349 favourable effect Effects 0.000 description 1
- 239000000945 filler Substances 0.000 description 1
- 239000001307 helium Substances 0.000 description 1
- 229910052734 helium Inorganic materials 0.000 description 1
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 1
- 239000001257 hydrogen Substances 0.000 description 1
- 229910052739 hydrogen Inorganic materials 0.000 description 1
- 230000008676 import Effects 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 229910001026 inconel Inorganic materials 0.000 description 1
- 238000010348 incorporation Methods 0.000 description 1
- 230000001939 inductive effect Effects 0.000 description 1
- 238000002347 injection Methods 0.000 description 1
- 239000007924 injection Substances 0.000 description 1
- 150000002500 ions Chemical class 0.000 description 1
- 230000000670 limiting effect Effects 0.000 description 1
- 230000007774 longterm Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 230000007246 mechanism Effects 0.000 description 1
- 229910044991 metal oxide Inorganic materials 0.000 description 1
- 150000004706 metal oxides Chemical class 0.000 description 1
- 229910052750 molybdenum Inorganic materials 0.000 description 1
- 239000011733 molybdenum Substances 0.000 description 1
- 238000004806 packaging method and process Methods 0.000 description 1
- 239000006069 physical mixture Substances 0.000 description 1
- 230000003334 potential effect Effects 0.000 description 1
- 238000007712 rapid solidification Methods 0.000 description 1
- 230000002829 reductive effect Effects 0.000 description 1
- 239000011214 refractory ceramic Substances 0.000 description 1
- 239000003870 refractory metal Substances 0.000 description 1
- 230000000717 retained effect Effects 0.000 description 1
- 230000002441 reversible effect Effects 0.000 description 1
- 230000003068 static effect Effects 0.000 description 1
- 239000010959 steel Substances 0.000 description 1
- 238000009864 tensile test Methods 0.000 description 1
- 239000010936 titanium Substances 0.000 description 1
- 229910052719 titanium Inorganic materials 0.000 description 1
- 229910003470 tongbaite Inorganic materials 0.000 description 1
- WFKWXMTUELFFGS-UHFFFAOYSA-N tungsten Chemical compound [W] WFKWXMTUELFFGS-UHFFFAOYSA-N 0.000 description 1
- 229910052721 tungsten Inorganic materials 0.000 description 1
- 239000010937 tungsten Substances 0.000 description 1
- 230000003313 weakening effect Effects 0.000 description 1
- 229910052726 zirconium Inorganic materials 0.000 description 1
Classifications
-
- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C4/00—Coating by spraying the coating material in the molten state, e.g. by flame, plasma or electric discharge
- C23C4/12—Coating by spraying the coating material in the molten state, e.g. by flame, plasma or electric discharge characterised by the method of spraying
- C23C4/134—Plasma spraying
Landscapes
- Engineering & Computer Science (AREA)
- Chemical & Material Sciences (AREA)
- Physics & Mathematics (AREA)
- Plasma & Fusion (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Materials Engineering (AREA)
- Mechanical Engineering (AREA)
- Metallurgy (AREA)
- Organic Chemistry (AREA)
- Coating By Spraying Or Casting (AREA)
- Manufacture Of Alloys Or Alloy Compounds (AREA)
- Laminated Bodies (AREA)
Abstract
RD-19,431 REINFORCED MICROLAMINATED
METAL-MATRIX-COMPOSITE STRUCTURE
ABSTRACT OF THE DISCLOSURE
Two separate plasma spray guns are employed simultaneously to spray a first metal from the first gun and to spray a second metal or a ceramic material from the second gun. The guns have a common aim point and the deposit formed has a swirl-like intermixed and interlocked structure.
METAL-MATRIX-COMPOSITE STRUCTURE
ABSTRACT OF THE DISCLOSURE
Two separate plasma spray guns are employed simultaneously to spray a first metal from the first gun and to spray a second metal or a ceramic material from the second gun. The guns have a common aim point and the deposit formed has a swirl-like intermixed and interlocked structure.
Description
-- 1 -- ' ~. ' ! i RD-19.431 ~ INFORCED MICROL~U~INATED
koET~L-ML~TRIX-CO ~ OSITE STR~CT~
CROSS-REFERENCE TO RELATED APPLICATION
The present invention is closely related to application Serial No. (Attorney docket RD- ), filed , the text of which is incorporated herein by reference.
BAC~GROUND OF THE INVENTION
The present invention relates generally to microlaminated metal-matrix-composite structures formed from deposits of a first metal either with a second metal, or with a ceramic material, in structures which have a generally laminated configuration. More specifically, it relates to laminar structures which are formed with metal matrices and with reinforcing members extending between the layers of the microlaminar struc~ure and to the methods of forming such structures.
The formation of generally laminar structures of two different materials has been described in the art. One such prior art publication is entitled "Production of Composite Structures By Low Pressure Plasma Deposition".
This article was published in Ceramic Engineering and Science Proceedings, Vol. 6, No. 7-8 (July/August 1985). This article describes structures which are similar to but not the same as the structures which are taught and claimed in the subject application. The prior art structures are formed by plasma deposition. For example, in Figures 7 and 8 of the article, structures are shown which have a generally laminar
koET~L-ML~TRIX-CO ~ OSITE STR~CT~
CROSS-REFERENCE TO RELATED APPLICATION
The present invention is closely related to application Serial No. (Attorney docket RD- ), filed , the text of which is incorporated herein by reference.
BAC~GROUND OF THE INVENTION
The present invention relates generally to microlaminated metal-matrix-composite structures formed from deposits of a first metal either with a second metal, or with a ceramic material, in structures which have a generally laminated configuration. More specifically, it relates to laminar structures which are formed with metal matrices and with reinforcing members extending between the layers of the microlaminar struc~ure and to the methods of forming such structures.
The formation of generally laminar structures of two different materials has been described in the art. One such prior art publication is entitled "Production of Composite Structures By Low Pressure Plasma Deposition".
This article was published in Ceramic Engineering and Science Proceedings, Vol. 6, No. 7-8 (July/August 1985). This article describes structures which are similar to but not the same as the structures which are taught and claimed in the subject application. The prior art structures are formed by plasma deposition. For example, in Figures 7 and 8 of the article, structures are shown which have a generally laminar
- 2 ~
f~ ` .7 ;J I J
Rp-19~431 configuration. In the structure of Figure 7, a superalloy is formed into a first set of laminae and chromium carbides, Cr3C2, forms the second or other set of laminae of the structure. In the structure of Figure 8, the laminar configuration of the alternating layers of superalloy and aluminum oxide are displayed.
Five other papers dealing with plasma sprayed coatings are as follows:
(1) R.~. Bunshah, C.V. Deshpandey, and B.P. O'Brien, "Microlaminate Composites - An Alte~native Approach to ~hermal Barrier Coatings", Paper presented at the Thermal Barrier Coatings Conference, NASA-Lewis, Cleveland, OH (May 1985).
(2) J.R. Rairden and D.M. Gray, "Study of Coordinated Two-Gun RSPD (Rapid Solidification Plasma Deposition) Processing to Achieve Size and Shape Control", GE Report No.
88~RD147 (June 1988) Class 1.
f~ ` .7 ;J I J
Rp-19~431 configuration. In the structure of Figure 7, a superalloy is formed into a first set of laminae and chromium carbides, Cr3C2, forms the second or other set of laminae of the structure. In the structure of Figure 8, the laminar configuration of the alternating layers of superalloy and aluminum oxide are displayed.
Five other papers dealing with plasma sprayed coatings are as follows:
(1) R.~. Bunshah, C.V. Deshpandey, and B.P. O'Brien, "Microlaminate Composites - An Alte~native Approach to ~hermal Barrier Coatings", Paper presented at the Thermal Barrier Coatings Conference, NASA-Lewis, Cleveland, OH (May 1985).
(2) J.R. Rairden and D.M. Gray, "Study of Coordinated Two-Gun RSPD (Rapid Solidification Plasma Deposition) Processing to Achieve Size and Shape Control", GE Report No.
88~RD147 (June 1988) Class 1.
(3) J.R. Rairden and D.M. Gray, "The Deposition of Turbine Blade Coat ~ngs Using Low-Pressure, Multigun Plasma Spray Processing~, published in the Trans. of the First International Conference on Plasma Surface Engineering, held at Garmisch-Partenkirchen, F~G (September 19 23, 1988).
(4) P.A. Siemers and W.B. Hillig, "Thermal-Barrier-Coated Turbine Blade Study", Report No. NASA CR-165351, SRD-25 81-083 (August 1981).
(5) G.P. Liang and J.W. Fairbanks, "Heat Transfer Investigation of Laminated Turbine Airfoils", Transactions of Gas Turbine Heat Transfer Symposium, pages 21-29, Winter Meeting of ASME, San Francisco (1978).
One of the problems which has been encountered in the formation and in the use of structures as disclosed in these articles is that they can lose some of their beneficial properties when they are subjected to extensive thermal cycling. By thermal cycling is meant that the structure is : ' . . . . ~ ~ ~ r.;
RD-19,431 heated as, for example, to a service temperature of over 1000C and then cooled to room temperature or even lower temperatures and then again heated and cooled, and etc. This thermal cycling has been recognized as a source of crack propagation in structures such as those described in the referenced article. Thus, where a relatively small crack develops in one of the ceramic lamina of a structure, the thermal cycling of the structure tends to cause propagation of the crack because of the stress induced due to the relatively large mismatch of the thermal coefficient of expansion of the metal member of the composite relative to the ceramic layers of the composite. The effect of propagation of a crack or cracks preferentially through one layer or laminar of the composite structure is to effectively cause a delamination of the structure. The impetus of driving force for such delamination is, as noted above, an extension of a crack formed, for example, in a ceramic layer of the composite through that layer and, accordingly, weakening and destroying the otherwise strong bond which may ~0 exist between the several laminae of the structure.
BRIEF STATEMENT OF THE INVENTION
It is, accordingly, one object of the present invention to provide microlaminated structures which minimize or eliminate the tendency of the structures to delaminate.
Another object is to provide microlaminated structures which display an ability to retain their laminar form.
Another object is to provide a microlaminated structure having a high strength to weight ratio.
Another object is to provide a microlaminated structure having low density and high elastic modulus.
RD-19,431 Another object is to provide a microlaminated structure havin~ controlled thermal expansion.
Another object is to provide a microlaminated structure having a controlled thermal conduction.
Another object is to provide a microlaminated structure having a controlled electrical conduction.
Another object is to provide a microlaminated structure which retains its laminar form while undergoing stress due to long-term ~hermal cycling or any other stress-inducing force.
Another object is to provide a method of limiting the growth of cracks in the microlaminae of composite laminar structures.
Other objects will be in part apparent and in part pointed out in the description which follows.
In one of its broader aspects, objects of the present invention can be achieved by providing a first plasma gun adapted to plasma spray deposit a first material, and by providing a second plasma gun adapted to plasma spray deposit a second material. These two independent guns are aimed at a common zone of a receiving surface and plasma spray deposit is formed in the ~one by the simultaneous combined spray deposit from both guns. It is found that the structure which is formed has a swirl configuration so that strands of reinforcement form extending between the laminae of the deposited structure and the resulting structure is capable of resisting delamination due to thermal cycling or other reasons. The swirl configuration of the structure is formed because the two distinct ingredients from the two separate guns are microlaminated or intermi~ed and finely interdisbursed as they are deposited so that they form a microlaminated structure.
By microlaminated and/or intermixed and/or a similar term as used herein is meant that the metal forms, in ~ Rn-14.43 J ~ .
essence, the continuous phase because the swirl formation of the deposited metal intermixes with ceramic to a degree which makes the metal dominate in the properties of the composite.
While the low pressure plasma spray process was used to form all of the materials described herein below, it would also be possible to use conventional atmospheric pressure processing to form the microlaminated structures described.
BRIEF DESCRIPTION OF THE DRA~INGS
The description which follows will be understood with greater clarity if reference is made to the accompanying drawings in which:
F~GUR~ 1 is a schematic illustration of the arrangement of two plasma spray guns relative to a substrate on which a combined plasma spray deposit is being formed;
FIGURE 2 is a side elevation (A) and end elevation (B) of a coupon on which plasma spray deposits were made;
FIGURES 3-5 are examples of the metallographic characteristics of a microlaminated structure, in this case, of NiCrAlY/Al2O3; and FIG~RE 6 is a graph in which percent expansion is plotted against temperature for a set of materials.
DETAILED DESCRIPTION OF THE INVENTION
One of the findings which is most significant in developing the structurally sound coatings is the finding that the simultaneous use of two different plasma spray guns having distinct ingredients in the separate guns results in the formation of a deposited layer having a distinctive structure. The distinctive structure is distinctive on both the macro and on the micro scale. In particular, the ~ RD-19.431 structure has a swirl-like intermixing of the different elements from the two guns so that there are essentially no continuous laminae present in the formed structure and there is, accordingly, no tendency for delamination to occur. This swirl-like structure is apparent on both a macro and micro scale. That is, the swirl-like structure can be seen with the unaided eye and can also be seen under magnification.
There are a number of parameters which are important in achieving the swirl-like intermixed and interlocked structure of a deposit made up of the two separate ingredients delivered to the surface from the separate guns.
A first parameter is the aim-point of the two guns.
Generally, it is desirable to have the aim-points of the guns coincide so that a deposit is being applied to the same area of the receiving surface from each gun. The aim-point may be determined, for example, by projecting an imaginary line through the nozzle of a gun and determining where the line will intercept the receiving surface at which the gun is aimed. An aim point can also be determined experimentally by observing where the center is located in a deposit from a stationary gun. It has been demonstrated that where the two aim points for the two guns coincide, the spray deposit which is delivered has a swirl-like configuration over the entire extent of the area where deposit is being made from each gun.
Another parameter is the angle of separation of the imaginary aimlines extending from the guns. This angle of separation is determined, in part, by the geometry of the guns themselves. For example, the EPI guns ~Electro Plasma, Inc., Irvine, CA) are physically larger than guns manufactured by Metco (Perkin Elmer Metco, Westbury, NY) so that the minimum angle of separation will be greater for a setup employing the EPI guns than for one employing the Metco guns. In general, we have found that it is desirable to use R~i - 19, 9 31 a minimum angle of separation so that the deposit angle from each gun is as near to perpendicular to the receiving surface as is physically possible for the guns employed. The use of the 90 deposition angle, that is where the imaginary aim line is approximately perpendicular to the receiving surface, results in the deposit of the most dense layers of deposited material.
My experience has shown that the deposition angle, that is the angle formed by the imaginary aimline and the surface to which the deposit is to be made, must be at least 70 to achieve a high density deposit.
At deposition angles of less than 70 the deposit becomes increasingly porous as the deposition angle is reduced. Swirl-like structure is found in such less dense deposits however. Where a controlled porosity is preferred, a deposition angle of less than 70 can be employed. Some experimentation to determine the degree of porosity ~hich is developed relative to the deposition angle may be employed to ensure that a desired porosity of a deposited layer is achieved. The use of porous thermal barrier coatings is feasible and the subject invention is particularly useful in improving the internal structure of the thermal barrier coatings so that laminar structures are avoided and interlocked swirly-types of structures are formed. The use of lower deposition angles ls deemed to have an influence on the bonding of a coating to a substrate surface and the formation of the more porous coatings may limit the bonding of coatings on a receiving substrate.
Another parameter in the formation of the layers of this invention is the distance from the gun to the substrate.
Generally, this distance ranges from about 8 to about 18 inches in low pressure plasma deposition and about 3 to 6 inches in atmospheric pressure plasma deposition. The distance is selected based upon spray pattern size desired.
~ ,) ,'`J RD-19 431 Larger spray patterns are developed when the guns are held at a greater distance from the receiving surface. Another factor concerned with the dis~ance is the heating of the substrate. Some heating is required to obtain a good bonding of the coating to the substrate and the shorter the distance of the gun to the substrate the greater the degree of heating of the substrate surface. This factor is one which can be determined with comparative ease by a few scoping tests to balance the requirements of a particular coating substrate combination. The factors involved are those indicated above, namely the degree of heating of the substrate where shorter distance increases the degree of heating, and the desired size of spray pattern on the receiving surface where greater distance increases the size of the spray pattern. Preheating a substrate, that is, before spray deposit starts, can be done very effectively with the plasma of a plasma gun.
The suppliers of guns which have been used successfully in the practice of the present in~ention are:
Electro Plasma Inc., 16842 Milliken Avenue, Irvine, CA
92714;
Perkin Elmer Metco, 1101 Prospect Avenue, Westbury, L.I., ~JY 11590; and Plasma-Technik, AG, Rigackerstrasse 21, 5610-Wohlen, Switzerland.
A further parameter involved in the practice of the invention is the size of the powder particles which are employed in forming the deposited layer. The particle sizes are selected based upon the melting characteristics of a material in the plasma. As an illustration, for metals such as nickel-based alloys, deposited at low pressure, a powder size of about 400 mesh or about 37 ~m with an average size of about 20 ~m has been found satisfactory. For lower melting point metals such as copper, a larger particle size such as a 270 mesh or about a 53 ~m size can be used successfully.
_ 9 _ ~ ; R~-19.431 Conversely, for refractory metals and ceramics, a powder size of 10-20 ~m is required in order to obtain a satisfactory melting of the particles and in order to form the swirly-type structure in the layer.
The primary criteria for the selection of a powder size is that the powder must be of a size so that it will melt when passing through the plasma and that it can be fed to the plasma gun using available powder feeders. In this regard, essentially any material that can be melted without decomposition can be plasma spray deposited.
An additional parameter concerned with the practice of the present method is the powder feed to and through the plasma gun. Powder feed mechanisms are commercially available and are suitable for use in connection with the present invention. Powder feed rates can be as high as 50 pounds per hour for a nickel-based alloy, for example. In general, feed rates of a few pounds per hour to as high as 20 pounds per hour are generally employed in the practice of the present inven ion.
Also, by using two guns as described here, graded composition coatings can be formed to tailor the properties of the coatings for particular applications. For instance, to minimize stress at a coating/substrate interface, the coating composition may be varied from high metal content at a metal substrate to high ceramic content at the outer surface; This can be done simply by varying the rates of powder feed to each gun during the deposition.
The carrier gas employed in connection with the invention has generally been argon. Flow rates used depend upon the particle size and density of the powder being fed and the velocity required for injection of the particles into the gun. Generally, the processing conditions recommended by the gun manufacturer are used. The flow rates of 10-40 standard cubic feet per hour would be typical in practicing ~ r'' '~ R~-l4.431 the present invention. The plasma gas employed in the operation of the plasma gun is typically a mixture of argon and helium or argon and hydrogen. Gas flow and gas composition for any particular powder are selected to achieve a desirable particle heating capability. Here it is conventional to do some scoping tests in order to provide the proper balance of parameters.
The method of practice of the invention and the combination of parameters found suitable are described illustratively in the following examples:
In this example, thermal barrier coatir,gs were deposited using two plasma spray guns mounted in a water-cooled low pressure chamber having dimensions of l.44 metersin diameter and l.37 meters in length for preparing plasma spray deposits. The guns were held stationary in positions having a common aim point and the receiving substrate was moved to produce the desired intermixed deposit on the chosen surface of the substrate. The guns were 80-kW EPI guns, Model 03CA. The guns were mounted on brackets that permitted the positioning of the guns at different angles with respect to a receiving substrate. The guns could be positioned as close as 9 centimeters apart. The guns could be angled over a wide range of angles so that the gun-aim-points were at the same area of the substrate and the spray patterns of the two separate guns overlapped in the manner schematically illustrated in Figure l.
The guns were positioned about 43.2 centimeters from the substrates on which the deposit was to be formed.
The powders employed in this study were as follows:
(1) Amdry 962, Ni-22Cr-lOAl-l.OY, obtained from Alloy Metals, Inc.
~ RD-19 43 (2) Amdry 995 powder having a composition of Co-32Ni-2lcr-8Al-o.sy~ also obtained from Alloy Metals, Inc.
(3) 105 SFP aluminum oxide powder obtained from Perkin-Elmer-Metco Corporation.
(4) ZrO2-8 wt% Y203 (-44~m + lO~m) obtained from Corning Glass Works.
The deposition conditions are given in Table I.
TABL~ I
1~
Plasma Deposition Conditions 80-kW Guns Anode 03-CA-110 Primary gas 122 l/min Ar Secondary gas 32 l/min He Powder feed gas 5.6 l/min Ar Power 1700 A, 44V
System pressure 60 mm Hg In this example, one gun was used to spray metal powder and the other gun was used to spray ceramic powder.
Two metal powders, NiCrAlY (Amdry 962) and CoNiCrAlY (Amdry 995) were sprayed in separate runs by the first gun. Two ceramics, Al2O3 (Metco 105SPF) and Zro2y2o3t were sprayed by the other gun.
Four runs were made as follows:
TABLR II
First Gun ~ssnn~_~n 1 NiCrAlY A12O3 35 2 CoNiCrAlY Al23 3 NiCrAlY ZrO2 Y2O3 9 CoNiCrAlY ZrO2 Y2O3 Rn-l9~4 As a measure of preparation for forming the plasma spray deposits, the substrates were first heated in the plasma flame to about 900C and the substrate surface was reverse transferred arc cleaned prior to commencing the coating deposition.
A number of substrates were employed to receive the deposits which were then subjected to thermocycling tests to test for delamination. These substrates were cast René ~0 coupons having configurations as illustrated in Figure 2.
These coupons were about lt2 inch in width, 1/4 inch in thickness, and about 1-3/4 inch in length. The coupons were supported from a holding rod extending from one end and welded thereto by Inconel 82 weld filler. A thermocouple hole was drilled in the end of the coupon opposite that from which the holding rod extended.
Cyclic oxidation tests were performed by exposing coupons alternatively in a static furnace at 1150C for S0 minutes and in room air for 10 minutes. Weight c~ange measurements were recorded during the 10-minute room air period of the oxidation cycle. Metallographic examinations were made by cutting transverse slices off the coupons.
From these tests, it was concluded that the Al2O3 is preferred to the ZrO2-Y2O3 as an oxide for incorporation in the MCrAlY metals, where M is Ni, Co, or some combination of Ni and Co. The composites containing the Al2O3 ceramic had superior strength and durability.
This example also demonstrated an important aspect of the subject method. That aspect is the ability to tailor the composite structures which are formed. By tailoring is meant that the ingredients themselves as well as the delivery of the molten oxide and molten metal to the receiving surface can be controlled and varied to impart to the formed deposit a desired set of properties within a broad envelope of , ~. . , ,:
R~-19.43 properties attainable with the combination of ingredients used.
In the above example, the coatings were prepared as thermal barrier coatings. The coatings containing the S zirconia were found to have lower durability and were also found to be subject to greater oxidation than the coatings containing the aluminum oxide.
Thermal conductivity tests showed that the NiCrAlY/alumina composite has about 40% of the thermal conductivity of NiCrAlY.
EXAMPLE 2: High Strength, Low Density, Free-Standing Microlaminated Composites of Xené 80/Al203 The procedures and apparatus of the above example were again used to form microlaminated composites.
In this case, an investigation was conducted of formation of microlaminated composites of René 80 with aluminum oxide to evaluate the potential of use of such material where high strength to weight ratio properties and high modulus properties are needed. Two specimen types of the microlaminated René 80/A1203 composites were made:
(1) Two deposits about 1.5 millimeters thick by 10 centimeters long by 3.8 centimeters in diameter on steel tube mandrels were formed. The René 80/A1203 volume ratios of the 25 tubes extended from 80-20 to 20-80. Five tube specimens having different ratios as follows were prepared: 80:20;
65:35; 50:50; 35:65; and 20:80. A gun separation angle corresponding to the angle theta of Figure 1 OI 45 was used to form tubes of each composition.
(2) A second set of tubes having René 80/Al~03 volume ratios were prepared having a gun angle of 10. These tubes had metal to oxide ratios of 65:35; 50:50; and 35:65. The second set of tubes was prepared to study the effect of the gun angle parameter on the microstructure of the tubular ~ RD-lqr43 deposits formed. In general as noted above, such tubular structures are formed by maintaining the plasma guns stationary and moving the tubular substrate both by rotation and by axial motion.
From the tube deposit tests made employing the René
80 and aluminum oxide, it was determined that at volume ratios of less than 50 to 50, the structural integrity of the deposit is poor. I found that the deposits with metal oxide volume ratios of 35 to 65 and 20 to 80 tended to break apart and this evidence of breakage was found even before the removal of the mandrel. The micrographs of Figures 3, 4, and 5 illustrate the three different ratios employed in forming the structures. Figure 3 is a micrograph at 400 magnification of the structure formed from 65 volume % Al2O3 15 and 35 volume % R-80. The structure of Figure 4 is formed from a composition of 50 volume % of Al2O3 and 50 volume percent R-80. The structure of Figure 5 is formed from a composition having 35 volume % Al2O3 and 65 volume percent René 80.
The René 80 powder employed in these experiments was a 400 mesh powder having an approximate average particle size of about 20 microns. The alloy René 80 is a commercially available alloy which has a composition by weight of 9.5 % cobalt, 14.0 % chromium, 3.0 % aluminum, 5.0 25 % titanium, 4.0 % molybdenum, 4.0 % tungsten, 0.03 weight %
zirconium, 0.015 % boron, and 0.17 % carbon, the balance of the alloy being nickel. The powder was obtained from Alloy Metals, Inc.
The aluminum oxide was 105 SPF aluminum oxide which was obtained from Perkin Elmer Metco Corporation.
The microstructures of the two deposits as illustrated in Figures 3, 4, and 5 demonstrate that the microstructure form is basically the swirly configuration which I have associated with the improvement in properties f` ~ Rr)- 1 9 . 4 31 which are found. Further, it is evident that from these microstructures that even though the phase distribution is not uniform, there is a fine interdispersion of the two phases. This is what gives the structure the benefit of the microlaminated construction which is responsible for the improved properties.
No gross microstructural differences were noted as a function of the angle between the guns. However, the properties data summarized in Table III do indicate that the guns' angle may be significant. Table III presents a summary of the experimental procedures employed in the study and experimental results which were found.
/
RD-l 9, ~31 --~r~ _ ,.
0~
o ~ ~ ~
~1~ ~3 H .. _ ~ ~ ~ ~ ~;;
a ~ ~ L ~
O ~ G " ~ ~
3 ~ a ~ _ ~ h 5 o 5 3~
s~ ~
~ RD-19.431 The compositions of the deposits ~ormed using an angle between the guns of 10 as determined by image analysis data tend to be closer to the compositions aimed for based on powder feed rate. In all of these deposits, except for the 50:50 deposit of René 80/Al203 using the 10 gun angle, the René 80 content was below the aimed composition. An angle between guns of 10 was used for the remainder of the test samples. Some additional information can be noted from the data presented in Table II. As noted in the Table, there was heat treatment applied to the deposits. The data in the Table indicates that there was little effect of heat treatment on the density of the deposits measured. However, the elastic modulus values and the 3 point bend strengths did increase as a result of the heat treatmen~ applied as listed in the Table.
Secondly, from the data listed in Table III, it can be observed that the expansion coefficients decrease and the electrical resi~stivities increase with increasing Al2O3 content. These data are consistent with the rule of mixtures consideration.
Plate deposits having a thickness of about 2.5 millimeters were formed on copper plate mandrels having dimensions of 15.2 x 15.2 centimeters. These deposits were also formed by holding the guns stationary and moving the plate substrate to receive the deposit. The plates were moved in both an x and y direction to expose the entire surface of the plate mandrel to the coincident plasma sprays.
In making these deposits, the angle between the guns was 10.
The René 80/Al203 volume ratios employed in making the microlaminated deposits on the plate mandrels were 80:20;
75:25; 65:35; and 50:50.
The data obtained from the preparation and testing of the plate deposits described and discussed above are set forth in Table IV immediately below:
: ~ ~ .Rn-19r43 TABLE IV
Tensile Test Properties of Microlaminated René 80/Al203 Plates Specimens heat treated 2 hr., 1250C, Ar except as noted Aim v/o Composition Test Temp. 0.2% YS UTS
René 80 Al23 (C~ (ksi) (ksi) R/A
RT llQ.7 0 560 107.5 0 710 113.4 0 860 88.1 88.4 Small 1010 35.5 36.3 Small RT 118.8 Small 560 98.1 0 710 111.3 111.3 Small 860 82.9 82.9 0 1010 36.0 36.1 Small RT 102.8 0 560 80.9 0 710 91.3 91.3 Small 860 77.6 77.6 Small 1010 39.2 39.4 Small 65* 35 RT 127.8 Small 560 115.5 0 710 113.9 116.7 Small 860 88.0 88.9 Small 1010 34.9 36.0 Small RT 71.5 0 560 66.0 0 710 No data 860 64.8 64.8Small 1010 36.7 0 100** RT 140 195 17.0 710 110 165 22.0 1010 30 40 10.0 * - Specimens not heat treated *~ - Representative data from previous studies 1" ' ' ,. - 'i,, RD-19.431 As is evident from the data included in the Table, the volume % ratios sought in preparing compositions were 80-20; 75-25; 65-35; 65-35 which specimen was not heat treated;
and 50-50. Data from a representative previous study is also included where René 80 would be 100%. The ratios listed in the Table were deposited using powder feed volume ratios as set forth. Sheet tensile specimens were cut from the plates.
The results of the tests from room temperature to 1010C are summarized in Table IV. These data can be compared with representative tensile data for rapidly solidified plasma deposited René 80 as set forth next to the 100% René 80 data.
There is a large decrease in axial tensile strength and ductility at lower temperatures for the microlaminated composites as compared to a rapidly solidified plasma deposited René 80 sample. The trend is for tensile strength to decrease with increasing A12O3 content. It should be noted that the 3 point bend strength values for the René 80 Al2O3 microlaminated specimens of Table III are significantly higher than the axial values. In addition, the axial tensile strengths of the microlaminated composites are almost equal to the rapidly solidified plasma deposited René 80 at 1010C.
The data suggests that there may be an advantage to the use of the microlaminated composite because of lower density and higher elastic modulus for those applications in which the low ductility can be tolerated.
From the foregoing, it is evident that a unique material may be tailored pursuant to the present invention to have high strength a~ low density, and accordingly to have a high strength to weight ratio. Also, it is evident that the density of the material can be tailored to a desired value by changing the properties of the ing edients used.
- ~o -~ R~-19 431 EX~æLE 3: Free-standing Microlaminated Composites of Invar:/A1~03 It became clear from the above examples that a wide variety of custom properties could be incorporated in various structures prepared pursuant to the present invention.
As a further illustration of this capability, a free standing material suitable for packaging for microelectronics was prepared. This material was to have a very low thermal coefficient of expansion and very low density. Invar metal was selected because it has a low coefficient of expansion. However, it is a weak metal and has a low modulus. It was sought to increase its strength and its modulus and to decrease its coefficient to expansion.
lS The apparatus and methods of the previous examples were again employed. Using these methods and apparatus, the properties of microlaminated composites of Invar/A1203were investigated to determine if the low coefficient of expansion properties could be retained in a lower density, higher elastic modulus and higher strength material. Plates of the microlaminated Invar/A1203composite were deposited using the following powder feed ratios by volume: 63:35; 50:50; and 35:65.
The properties of these materials were measured as described above and these properties are summarized in Table V which is set forth immediately below.
.i RD- l 9, 4 31 ~'' ~''1'1 o~ ~ 3--~ 3 3 ~
~ ~ . 3 1 ~ ~ a . : ~ `
; i R~-19,4 The microlaminated sample of 35 Invar/65 Al2O3 formed on the plate was found to be extremely brittle and so brittle, in factr that i~ could not be machined into a mechanical test specimen. From the Table V, it can be seen that the Invar content of these microlaminated plates was lower than the target content and, accordingly, was lower than expected based on the powder feed rate for all the specimens. This lower figure for the metal component of the composite is similar to the data already discussed for the microlaminated composition containing René 80 and Al2O3.
However, this lower value can be overcome by adjusting the respective feed rates to feed a higher level of metal to bring the density and other properties to a desired level within the range of densities available and consistent with achieving a desired overall set of properties.
The elastic modulus properties of the microlaminated Invar/Al2O3 specimens are about 50% higher than the elastic modulus of Invar and the electrical resistivity of the microlaminated samples was observed to increase with increasing Al2O3 content.
A minimum in expansion coefficient at a volume ratio of about 40% Invar/60% Al2O3 was indicated. The data obtained indicate that the microlaminated Invar/A12O3 25 compositions can be identified with a thermal expansion ;-coefficient approximating that of Invar.
From the data obtained from this evaluation of the microlaminated Invar/Al2O3 compositions, it appears highly probable that material can be developed from these ingredients which display low density, low thermal expansion, high elastic modulus, and reasonable strength properties as compared to Invar per se.
RD-19.43L
EXA~ 4: Free-standing Microlaminated Composites of - Copper and A1203 The properties of microlaminated copper/aluminum oxide deposits were explored for potential application and power hybrid microelectronics. A series of microlaminated samples of copper and aluminum oxide were formed on plates as described above in Example 3. The deposits on the plates were formed using feeder/rate volume % ratios of 65:35;
50:50; and 35:65. The properties of these materials are summarized in Table VI.
-'',., ~ ` ~
.,''',` l `- ~` " ' l ~ !
., .
-- 2~1 --, ~, ,,~,, N 4 ~1 0 ~; ~o Y Y ~ o~
A = , . ~ ~ _ ~ _ Eo ~"A ~
~ !" ~ 1~ ~ 8 g ~
~ - R~-l9~a3l ,~. .., , . ~, -For these plates, the image analysis data appear to be misleading. Based on the measured density values, the copper content of the 65 volume % copper, 35 volume % aluminum oxide, and of the 50 volume % copper and 50 volume % Al2O3 plates are higher than the aimed compositions.
It can be noted from the data included in Table VI
that the electrical resistivity values increase and the thermal expansion coefficient values decrease systematically with increasing Al2O3 content. The elastic modulus values reflect the Al2O3 content in the microlaminated composites.
From the foregoing, it is evident that metal matrix composite structures can be formed by low pressure plasma deposition using the coordinated two-gun process of the subject invention.
By microlaminated and~or intermixed and/or terms of similar import as used herein it meant that the metal forms, in essence, the continuous phase because the swirl formation of the deposited metal intermixes with ceramic to a degree which makes the metal dominate in the properties of the composite.
These deposits can be used as coatings or as free standing bodies. The structures can be employed in a number of specific applications. For example, they can be employed in oxidation and hot corroslon resistant materials. Further, they can be employed as thermal barriers or insulating barrier materials. Further, the structures can be employed as structural materials per se.
The metal matrix composites employing the swirl-type microstructure of the present invention are a class ofadvanced materials that hold promise for meeting a wide variety of industrial requirements. A number of potential property advantages of such structures make them particularly useful in such applications. Among these advan~ages are the , ~ ,.
~ RD-19.43 high strength to weight ratio; low density; high elastic modulus; controlled thermal expansion; and controlled thermal and electrical conduction. An important aspect of the invention is that materials can be tailored to have a desired S combination of these advantageous properties.
One of the processing techniques which is particularly suitable for the formation of structures as provided pursuant to the present invention is the low pressure plasma deposition techniques such as are taught in the patent 4,603,568. The text of the patent is incorporated herein by reference.
A distinction from the 4,603,568 teaching as carried out in the present invention is that the metal sprayed from one gun is combined instantaneously with the ceramic sprayed from the other gun in a low pressure plasma deposition chamber where both guns are aimed simultaneously at the same deposit zone of a receiving surface. ~hat was achieved by the examples recited above wa~ a simultaneous bombardment of the substrate ~ith splatters of both materials so that the two phases were interminqled and combined into a fine swirly anisotropic distribution.
The microstructure formed was deemed to have durability because of the effect of minimizing the tendency to form extensive continuous layers of ceramic. Such continuous layers of ceramic are subject to forming planes of weakness particularly during thermal cycling. The work per~ormed, as represented by Examples referred to above, demonstrated the potential of forming free standing composites and coating composites using the coordinated two gun low pressure plasma deposition processing. It was thus demonstrated that a fine interdispersion of the two material phases could be achieved and that these phases are present in a swirly intermingled microstructure. The property data obtained indicate the potential of this system for tailoring RD-l 9. a31 composite materials using the rapid solidification plasma deposition simultaneous processing of metal and ceramic materials to meet a variety of application requirements. In this regard, it has been demonstrated that density values can be lowered by combining ceramic with metal. Further, elas~ic modulus values of the composite can be increased by altering proportions of the deposited materials, and particularly by increasing the ceramic component of the composite. The overall thermal expansion coefficients of the deposit can be decreased by employing the combination of metal and ceramic materials. The control of coefficient is illustrated in the graph of Figure 6. Thermal conductivity values can be increased or decreased by judicious choice of material components for a composite system.
The use of the system makes a number of processing advantages available and these include the use of the optimal spray parameters for each of the materials. In other words, the optimal spray parameters for the metal are going to be different from the optimal spray parameters for the ceramic.
However, since the two guns are employed simultaneously but independently, the operating parameters of the guns can be adjusted to the best parameters for the material processed through that gun.
It will be understood that the invention is not limited to the employment of only two guns but that more than two guns can be employed to achieve dissimilar surprisingly advantageous structures through the development of the swirly intermixed microstructure.
Another advantage of the simultaneous two-gun processing is that the deposition angles of each material can be varied to maximize the degree to which the microstructure is intermixed and swirly and hence improved in durability.
- This is another favorable property of the deposit.
RD-14,431 A further advantage is that separate powder feeders can be used for each material to eliminate potential problem of separation due to density differences during processing when a physical mixture of two materials is used.
One of the problems which has been encountered in the formation and in the use of structures as disclosed in these articles is that they can lose some of their beneficial properties when they are subjected to extensive thermal cycling. By thermal cycling is meant that the structure is : ' . . . . ~ ~ ~ r.;
RD-19,431 heated as, for example, to a service temperature of over 1000C and then cooled to room temperature or even lower temperatures and then again heated and cooled, and etc. This thermal cycling has been recognized as a source of crack propagation in structures such as those described in the referenced article. Thus, where a relatively small crack develops in one of the ceramic lamina of a structure, the thermal cycling of the structure tends to cause propagation of the crack because of the stress induced due to the relatively large mismatch of the thermal coefficient of expansion of the metal member of the composite relative to the ceramic layers of the composite. The effect of propagation of a crack or cracks preferentially through one layer or laminar of the composite structure is to effectively cause a delamination of the structure. The impetus of driving force for such delamination is, as noted above, an extension of a crack formed, for example, in a ceramic layer of the composite through that layer and, accordingly, weakening and destroying the otherwise strong bond which may ~0 exist between the several laminae of the structure.
BRIEF STATEMENT OF THE INVENTION
It is, accordingly, one object of the present invention to provide microlaminated structures which minimize or eliminate the tendency of the structures to delaminate.
Another object is to provide microlaminated structures which display an ability to retain their laminar form.
Another object is to provide a microlaminated structure having a high strength to weight ratio.
Another object is to provide a microlaminated structure having low density and high elastic modulus.
RD-19,431 Another object is to provide a microlaminated structure havin~ controlled thermal expansion.
Another object is to provide a microlaminated structure having a controlled thermal conduction.
Another object is to provide a microlaminated structure having a controlled electrical conduction.
Another object is to provide a microlaminated structure which retains its laminar form while undergoing stress due to long-term ~hermal cycling or any other stress-inducing force.
Another object is to provide a method of limiting the growth of cracks in the microlaminae of composite laminar structures.
Other objects will be in part apparent and in part pointed out in the description which follows.
In one of its broader aspects, objects of the present invention can be achieved by providing a first plasma gun adapted to plasma spray deposit a first material, and by providing a second plasma gun adapted to plasma spray deposit a second material. These two independent guns are aimed at a common zone of a receiving surface and plasma spray deposit is formed in the ~one by the simultaneous combined spray deposit from both guns. It is found that the structure which is formed has a swirl configuration so that strands of reinforcement form extending between the laminae of the deposited structure and the resulting structure is capable of resisting delamination due to thermal cycling or other reasons. The swirl configuration of the structure is formed because the two distinct ingredients from the two separate guns are microlaminated or intermi~ed and finely interdisbursed as they are deposited so that they form a microlaminated structure.
By microlaminated and/or intermixed and/or a similar term as used herein is meant that the metal forms, in ~ Rn-14.43 J ~ .
essence, the continuous phase because the swirl formation of the deposited metal intermixes with ceramic to a degree which makes the metal dominate in the properties of the composite.
While the low pressure plasma spray process was used to form all of the materials described herein below, it would also be possible to use conventional atmospheric pressure processing to form the microlaminated structures described.
BRIEF DESCRIPTION OF THE DRA~INGS
The description which follows will be understood with greater clarity if reference is made to the accompanying drawings in which:
F~GUR~ 1 is a schematic illustration of the arrangement of two plasma spray guns relative to a substrate on which a combined plasma spray deposit is being formed;
FIGURE 2 is a side elevation (A) and end elevation (B) of a coupon on which plasma spray deposits were made;
FIGURES 3-5 are examples of the metallographic characteristics of a microlaminated structure, in this case, of NiCrAlY/Al2O3; and FIG~RE 6 is a graph in which percent expansion is plotted against temperature for a set of materials.
DETAILED DESCRIPTION OF THE INVENTION
One of the findings which is most significant in developing the structurally sound coatings is the finding that the simultaneous use of two different plasma spray guns having distinct ingredients in the separate guns results in the formation of a deposited layer having a distinctive structure. The distinctive structure is distinctive on both the macro and on the micro scale. In particular, the ~ RD-19.431 structure has a swirl-like intermixing of the different elements from the two guns so that there are essentially no continuous laminae present in the formed structure and there is, accordingly, no tendency for delamination to occur. This swirl-like structure is apparent on both a macro and micro scale. That is, the swirl-like structure can be seen with the unaided eye and can also be seen under magnification.
There are a number of parameters which are important in achieving the swirl-like intermixed and interlocked structure of a deposit made up of the two separate ingredients delivered to the surface from the separate guns.
A first parameter is the aim-point of the two guns.
Generally, it is desirable to have the aim-points of the guns coincide so that a deposit is being applied to the same area of the receiving surface from each gun. The aim-point may be determined, for example, by projecting an imaginary line through the nozzle of a gun and determining where the line will intercept the receiving surface at which the gun is aimed. An aim point can also be determined experimentally by observing where the center is located in a deposit from a stationary gun. It has been demonstrated that where the two aim points for the two guns coincide, the spray deposit which is delivered has a swirl-like configuration over the entire extent of the area where deposit is being made from each gun.
Another parameter is the angle of separation of the imaginary aimlines extending from the guns. This angle of separation is determined, in part, by the geometry of the guns themselves. For example, the EPI guns ~Electro Plasma, Inc., Irvine, CA) are physically larger than guns manufactured by Metco (Perkin Elmer Metco, Westbury, NY) so that the minimum angle of separation will be greater for a setup employing the EPI guns than for one employing the Metco guns. In general, we have found that it is desirable to use R~i - 19, 9 31 a minimum angle of separation so that the deposit angle from each gun is as near to perpendicular to the receiving surface as is physically possible for the guns employed. The use of the 90 deposition angle, that is where the imaginary aim line is approximately perpendicular to the receiving surface, results in the deposit of the most dense layers of deposited material.
My experience has shown that the deposition angle, that is the angle formed by the imaginary aimline and the surface to which the deposit is to be made, must be at least 70 to achieve a high density deposit.
At deposition angles of less than 70 the deposit becomes increasingly porous as the deposition angle is reduced. Swirl-like structure is found in such less dense deposits however. Where a controlled porosity is preferred, a deposition angle of less than 70 can be employed. Some experimentation to determine the degree of porosity ~hich is developed relative to the deposition angle may be employed to ensure that a desired porosity of a deposited layer is achieved. The use of porous thermal barrier coatings is feasible and the subject invention is particularly useful in improving the internal structure of the thermal barrier coatings so that laminar structures are avoided and interlocked swirly-types of structures are formed. The use of lower deposition angles ls deemed to have an influence on the bonding of a coating to a substrate surface and the formation of the more porous coatings may limit the bonding of coatings on a receiving substrate.
Another parameter in the formation of the layers of this invention is the distance from the gun to the substrate.
Generally, this distance ranges from about 8 to about 18 inches in low pressure plasma deposition and about 3 to 6 inches in atmospheric pressure plasma deposition. The distance is selected based upon spray pattern size desired.
~ ,) ,'`J RD-19 431 Larger spray patterns are developed when the guns are held at a greater distance from the receiving surface. Another factor concerned with the dis~ance is the heating of the substrate. Some heating is required to obtain a good bonding of the coating to the substrate and the shorter the distance of the gun to the substrate the greater the degree of heating of the substrate surface. This factor is one which can be determined with comparative ease by a few scoping tests to balance the requirements of a particular coating substrate combination. The factors involved are those indicated above, namely the degree of heating of the substrate where shorter distance increases the degree of heating, and the desired size of spray pattern on the receiving surface where greater distance increases the size of the spray pattern. Preheating a substrate, that is, before spray deposit starts, can be done very effectively with the plasma of a plasma gun.
The suppliers of guns which have been used successfully in the practice of the present in~ention are:
Electro Plasma Inc., 16842 Milliken Avenue, Irvine, CA
92714;
Perkin Elmer Metco, 1101 Prospect Avenue, Westbury, L.I., ~JY 11590; and Plasma-Technik, AG, Rigackerstrasse 21, 5610-Wohlen, Switzerland.
A further parameter involved in the practice of the invention is the size of the powder particles which are employed in forming the deposited layer. The particle sizes are selected based upon the melting characteristics of a material in the plasma. As an illustration, for metals such as nickel-based alloys, deposited at low pressure, a powder size of about 400 mesh or about 37 ~m with an average size of about 20 ~m has been found satisfactory. For lower melting point metals such as copper, a larger particle size such as a 270 mesh or about a 53 ~m size can be used successfully.
_ 9 _ ~ ; R~-19.431 Conversely, for refractory metals and ceramics, a powder size of 10-20 ~m is required in order to obtain a satisfactory melting of the particles and in order to form the swirly-type structure in the layer.
The primary criteria for the selection of a powder size is that the powder must be of a size so that it will melt when passing through the plasma and that it can be fed to the plasma gun using available powder feeders. In this regard, essentially any material that can be melted without decomposition can be plasma spray deposited.
An additional parameter concerned with the practice of the present method is the powder feed to and through the plasma gun. Powder feed mechanisms are commercially available and are suitable for use in connection with the present invention. Powder feed rates can be as high as 50 pounds per hour for a nickel-based alloy, for example. In general, feed rates of a few pounds per hour to as high as 20 pounds per hour are generally employed in the practice of the present inven ion.
Also, by using two guns as described here, graded composition coatings can be formed to tailor the properties of the coatings for particular applications. For instance, to minimize stress at a coating/substrate interface, the coating composition may be varied from high metal content at a metal substrate to high ceramic content at the outer surface; This can be done simply by varying the rates of powder feed to each gun during the deposition.
The carrier gas employed in connection with the invention has generally been argon. Flow rates used depend upon the particle size and density of the powder being fed and the velocity required for injection of the particles into the gun. Generally, the processing conditions recommended by the gun manufacturer are used. The flow rates of 10-40 standard cubic feet per hour would be typical in practicing ~ r'' '~ R~-l4.431 the present invention. The plasma gas employed in the operation of the plasma gun is typically a mixture of argon and helium or argon and hydrogen. Gas flow and gas composition for any particular powder are selected to achieve a desirable particle heating capability. Here it is conventional to do some scoping tests in order to provide the proper balance of parameters.
The method of practice of the invention and the combination of parameters found suitable are described illustratively in the following examples:
In this example, thermal barrier coatir,gs were deposited using two plasma spray guns mounted in a water-cooled low pressure chamber having dimensions of l.44 metersin diameter and l.37 meters in length for preparing plasma spray deposits. The guns were held stationary in positions having a common aim point and the receiving substrate was moved to produce the desired intermixed deposit on the chosen surface of the substrate. The guns were 80-kW EPI guns, Model 03CA. The guns were mounted on brackets that permitted the positioning of the guns at different angles with respect to a receiving substrate. The guns could be positioned as close as 9 centimeters apart. The guns could be angled over a wide range of angles so that the gun-aim-points were at the same area of the substrate and the spray patterns of the two separate guns overlapped in the manner schematically illustrated in Figure l.
The guns were positioned about 43.2 centimeters from the substrates on which the deposit was to be formed.
The powders employed in this study were as follows:
(1) Amdry 962, Ni-22Cr-lOAl-l.OY, obtained from Alloy Metals, Inc.
~ RD-19 43 (2) Amdry 995 powder having a composition of Co-32Ni-2lcr-8Al-o.sy~ also obtained from Alloy Metals, Inc.
(3) 105 SFP aluminum oxide powder obtained from Perkin-Elmer-Metco Corporation.
(4) ZrO2-8 wt% Y203 (-44~m + lO~m) obtained from Corning Glass Works.
The deposition conditions are given in Table I.
TABL~ I
1~
Plasma Deposition Conditions 80-kW Guns Anode 03-CA-110 Primary gas 122 l/min Ar Secondary gas 32 l/min He Powder feed gas 5.6 l/min Ar Power 1700 A, 44V
System pressure 60 mm Hg In this example, one gun was used to spray metal powder and the other gun was used to spray ceramic powder.
Two metal powders, NiCrAlY (Amdry 962) and CoNiCrAlY (Amdry 995) were sprayed in separate runs by the first gun. Two ceramics, Al2O3 (Metco 105SPF) and Zro2y2o3t were sprayed by the other gun.
Four runs were made as follows:
TABLR II
First Gun ~ssnn~_~n 1 NiCrAlY A12O3 35 2 CoNiCrAlY Al23 3 NiCrAlY ZrO2 Y2O3 9 CoNiCrAlY ZrO2 Y2O3 Rn-l9~4 As a measure of preparation for forming the plasma spray deposits, the substrates were first heated in the plasma flame to about 900C and the substrate surface was reverse transferred arc cleaned prior to commencing the coating deposition.
A number of substrates were employed to receive the deposits which were then subjected to thermocycling tests to test for delamination. These substrates were cast René ~0 coupons having configurations as illustrated in Figure 2.
These coupons were about lt2 inch in width, 1/4 inch in thickness, and about 1-3/4 inch in length. The coupons were supported from a holding rod extending from one end and welded thereto by Inconel 82 weld filler. A thermocouple hole was drilled in the end of the coupon opposite that from which the holding rod extended.
Cyclic oxidation tests were performed by exposing coupons alternatively in a static furnace at 1150C for S0 minutes and in room air for 10 minutes. Weight c~ange measurements were recorded during the 10-minute room air period of the oxidation cycle. Metallographic examinations were made by cutting transverse slices off the coupons.
From these tests, it was concluded that the Al2O3 is preferred to the ZrO2-Y2O3 as an oxide for incorporation in the MCrAlY metals, where M is Ni, Co, or some combination of Ni and Co. The composites containing the Al2O3 ceramic had superior strength and durability.
This example also demonstrated an important aspect of the subject method. That aspect is the ability to tailor the composite structures which are formed. By tailoring is meant that the ingredients themselves as well as the delivery of the molten oxide and molten metal to the receiving surface can be controlled and varied to impart to the formed deposit a desired set of properties within a broad envelope of , ~. . , ,:
R~-19.43 properties attainable with the combination of ingredients used.
In the above example, the coatings were prepared as thermal barrier coatings. The coatings containing the S zirconia were found to have lower durability and were also found to be subject to greater oxidation than the coatings containing the aluminum oxide.
Thermal conductivity tests showed that the NiCrAlY/alumina composite has about 40% of the thermal conductivity of NiCrAlY.
EXAMPLE 2: High Strength, Low Density, Free-Standing Microlaminated Composites of Xené 80/Al203 The procedures and apparatus of the above example were again used to form microlaminated composites.
In this case, an investigation was conducted of formation of microlaminated composites of René 80 with aluminum oxide to evaluate the potential of use of such material where high strength to weight ratio properties and high modulus properties are needed. Two specimen types of the microlaminated René 80/A1203 composites were made:
(1) Two deposits about 1.5 millimeters thick by 10 centimeters long by 3.8 centimeters in diameter on steel tube mandrels were formed. The René 80/A1203 volume ratios of the 25 tubes extended from 80-20 to 20-80. Five tube specimens having different ratios as follows were prepared: 80:20;
65:35; 50:50; 35:65; and 20:80. A gun separation angle corresponding to the angle theta of Figure 1 OI 45 was used to form tubes of each composition.
(2) A second set of tubes having René 80/Al~03 volume ratios were prepared having a gun angle of 10. These tubes had metal to oxide ratios of 65:35; 50:50; and 35:65. The second set of tubes was prepared to study the effect of the gun angle parameter on the microstructure of the tubular ~ RD-lqr43 deposits formed. In general as noted above, such tubular structures are formed by maintaining the plasma guns stationary and moving the tubular substrate both by rotation and by axial motion.
From the tube deposit tests made employing the René
80 and aluminum oxide, it was determined that at volume ratios of less than 50 to 50, the structural integrity of the deposit is poor. I found that the deposits with metal oxide volume ratios of 35 to 65 and 20 to 80 tended to break apart and this evidence of breakage was found even before the removal of the mandrel. The micrographs of Figures 3, 4, and 5 illustrate the three different ratios employed in forming the structures. Figure 3 is a micrograph at 400 magnification of the structure formed from 65 volume % Al2O3 15 and 35 volume % R-80. The structure of Figure 4 is formed from a composition of 50 volume % of Al2O3 and 50 volume percent R-80. The structure of Figure 5 is formed from a composition having 35 volume % Al2O3 and 65 volume percent René 80.
The René 80 powder employed in these experiments was a 400 mesh powder having an approximate average particle size of about 20 microns. The alloy René 80 is a commercially available alloy which has a composition by weight of 9.5 % cobalt, 14.0 % chromium, 3.0 % aluminum, 5.0 25 % titanium, 4.0 % molybdenum, 4.0 % tungsten, 0.03 weight %
zirconium, 0.015 % boron, and 0.17 % carbon, the balance of the alloy being nickel. The powder was obtained from Alloy Metals, Inc.
The aluminum oxide was 105 SPF aluminum oxide which was obtained from Perkin Elmer Metco Corporation.
The microstructures of the two deposits as illustrated in Figures 3, 4, and 5 demonstrate that the microstructure form is basically the swirly configuration which I have associated with the improvement in properties f` ~ Rr)- 1 9 . 4 31 which are found. Further, it is evident that from these microstructures that even though the phase distribution is not uniform, there is a fine interdispersion of the two phases. This is what gives the structure the benefit of the microlaminated construction which is responsible for the improved properties.
No gross microstructural differences were noted as a function of the angle between the guns. However, the properties data summarized in Table III do indicate that the guns' angle may be significant. Table III presents a summary of the experimental procedures employed in the study and experimental results which were found.
/
RD-l 9, ~31 --~r~ _ ,.
0~
o ~ ~ ~
~1~ ~3 H .. _ ~ ~ ~ ~ ~;;
a ~ ~ L ~
O ~ G " ~ ~
3 ~ a ~ _ ~ h 5 o 5 3~
s~ ~
~ RD-19.431 The compositions of the deposits ~ormed using an angle between the guns of 10 as determined by image analysis data tend to be closer to the compositions aimed for based on powder feed rate. In all of these deposits, except for the 50:50 deposit of René 80/Al203 using the 10 gun angle, the René 80 content was below the aimed composition. An angle between guns of 10 was used for the remainder of the test samples. Some additional information can be noted from the data presented in Table II. As noted in the Table, there was heat treatment applied to the deposits. The data in the Table indicates that there was little effect of heat treatment on the density of the deposits measured. However, the elastic modulus values and the 3 point bend strengths did increase as a result of the heat treatmen~ applied as listed in the Table.
Secondly, from the data listed in Table III, it can be observed that the expansion coefficients decrease and the electrical resi~stivities increase with increasing Al2O3 content. These data are consistent with the rule of mixtures consideration.
Plate deposits having a thickness of about 2.5 millimeters were formed on copper plate mandrels having dimensions of 15.2 x 15.2 centimeters. These deposits were also formed by holding the guns stationary and moving the plate substrate to receive the deposit. The plates were moved in both an x and y direction to expose the entire surface of the plate mandrel to the coincident plasma sprays.
In making these deposits, the angle between the guns was 10.
The René 80/Al203 volume ratios employed in making the microlaminated deposits on the plate mandrels were 80:20;
75:25; 65:35; and 50:50.
The data obtained from the preparation and testing of the plate deposits described and discussed above are set forth in Table IV immediately below:
: ~ ~ .Rn-19r43 TABLE IV
Tensile Test Properties of Microlaminated René 80/Al203 Plates Specimens heat treated 2 hr., 1250C, Ar except as noted Aim v/o Composition Test Temp. 0.2% YS UTS
René 80 Al23 (C~ (ksi) (ksi) R/A
RT llQ.7 0 560 107.5 0 710 113.4 0 860 88.1 88.4 Small 1010 35.5 36.3 Small RT 118.8 Small 560 98.1 0 710 111.3 111.3 Small 860 82.9 82.9 0 1010 36.0 36.1 Small RT 102.8 0 560 80.9 0 710 91.3 91.3 Small 860 77.6 77.6 Small 1010 39.2 39.4 Small 65* 35 RT 127.8 Small 560 115.5 0 710 113.9 116.7 Small 860 88.0 88.9 Small 1010 34.9 36.0 Small RT 71.5 0 560 66.0 0 710 No data 860 64.8 64.8Small 1010 36.7 0 100** RT 140 195 17.0 710 110 165 22.0 1010 30 40 10.0 * - Specimens not heat treated *~ - Representative data from previous studies 1" ' ' ,. - 'i,, RD-19.431 As is evident from the data included in the Table, the volume % ratios sought in preparing compositions were 80-20; 75-25; 65-35; 65-35 which specimen was not heat treated;
and 50-50. Data from a representative previous study is also included where René 80 would be 100%. The ratios listed in the Table were deposited using powder feed volume ratios as set forth. Sheet tensile specimens were cut from the plates.
The results of the tests from room temperature to 1010C are summarized in Table IV. These data can be compared with representative tensile data for rapidly solidified plasma deposited René 80 as set forth next to the 100% René 80 data.
There is a large decrease in axial tensile strength and ductility at lower temperatures for the microlaminated composites as compared to a rapidly solidified plasma deposited René 80 sample. The trend is for tensile strength to decrease with increasing A12O3 content. It should be noted that the 3 point bend strength values for the René 80 Al2O3 microlaminated specimens of Table III are significantly higher than the axial values. In addition, the axial tensile strengths of the microlaminated composites are almost equal to the rapidly solidified plasma deposited René 80 at 1010C.
The data suggests that there may be an advantage to the use of the microlaminated composite because of lower density and higher elastic modulus for those applications in which the low ductility can be tolerated.
From the foregoing, it is evident that a unique material may be tailored pursuant to the present invention to have high strength a~ low density, and accordingly to have a high strength to weight ratio. Also, it is evident that the density of the material can be tailored to a desired value by changing the properties of the ing edients used.
- ~o -~ R~-19 431 EX~æLE 3: Free-standing Microlaminated Composites of Invar:/A1~03 It became clear from the above examples that a wide variety of custom properties could be incorporated in various structures prepared pursuant to the present invention.
As a further illustration of this capability, a free standing material suitable for packaging for microelectronics was prepared. This material was to have a very low thermal coefficient of expansion and very low density. Invar metal was selected because it has a low coefficient of expansion. However, it is a weak metal and has a low modulus. It was sought to increase its strength and its modulus and to decrease its coefficient to expansion.
lS The apparatus and methods of the previous examples were again employed. Using these methods and apparatus, the properties of microlaminated composites of Invar/A1203were investigated to determine if the low coefficient of expansion properties could be retained in a lower density, higher elastic modulus and higher strength material. Plates of the microlaminated Invar/A1203composite were deposited using the following powder feed ratios by volume: 63:35; 50:50; and 35:65.
The properties of these materials were measured as described above and these properties are summarized in Table V which is set forth immediately below.
.i RD- l 9, 4 31 ~'' ~''1'1 o~ ~ 3--~ 3 3 ~
~ ~ . 3 1 ~ ~ a . : ~ `
; i R~-19,4 The microlaminated sample of 35 Invar/65 Al2O3 formed on the plate was found to be extremely brittle and so brittle, in factr that i~ could not be machined into a mechanical test specimen. From the Table V, it can be seen that the Invar content of these microlaminated plates was lower than the target content and, accordingly, was lower than expected based on the powder feed rate for all the specimens. This lower figure for the metal component of the composite is similar to the data already discussed for the microlaminated composition containing René 80 and Al2O3.
However, this lower value can be overcome by adjusting the respective feed rates to feed a higher level of metal to bring the density and other properties to a desired level within the range of densities available and consistent with achieving a desired overall set of properties.
The elastic modulus properties of the microlaminated Invar/Al2O3 specimens are about 50% higher than the elastic modulus of Invar and the electrical resistivity of the microlaminated samples was observed to increase with increasing Al2O3 content.
A minimum in expansion coefficient at a volume ratio of about 40% Invar/60% Al2O3 was indicated. The data obtained indicate that the microlaminated Invar/A12O3 25 compositions can be identified with a thermal expansion ;-coefficient approximating that of Invar.
From the data obtained from this evaluation of the microlaminated Invar/Al2O3 compositions, it appears highly probable that material can be developed from these ingredients which display low density, low thermal expansion, high elastic modulus, and reasonable strength properties as compared to Invar per se.
RD-19.43L
EXA~ 4: Free-standing Microlaminated Composites of - Copper and A1203 The properties of microlaminated copper/aluminum oxide deposits were explored for potential application and power hybrid microelectronics. A series of microlaminated samples of copper and aluminum oxide were formed on plates as described above in Example 3. The deposits on the plates were formed using feeder/rate volume % ratios of 65:35;
50:50; and 35:65. The properties of these materials are summarized in Table VI.
-'',., ~ ` ~
.,''',` l `- ~` " ' l ~ !
., .
-- 2~1 --, ~, ,,~,, N 4 ~1 0 ~; ~o Y Y ~ o~
A = , . ~ ~ _ ~ _ Eo ~"A ~
~ !" ~ 1~ ~ 8 g ~
~ - R~-l9~a3l ,~. .., , . ~, -For these plates, the image analysis data appear to be misleading. Based on the measured density values, the copper content of the 65 volume % copper, 35 volume % aluminum oxide, and of the 50 volume % copper and 50 volume % Al2O3 plates are higher than the aimed compositions.
It can be noted from the data included in Table VI
that the electrical resistivity values increase and the thermal expansion coefficient values decrease systematically with increasing Al2O3 content. The elastic modulus values reflect the Al2O3 content in the microlaminated composites.
From the foregoing, it is evident that metal matrix composite structures can be formed by low pressure plasma deposition using the coordinated two-gun process of the subject invention.
By microlaminated and~or intermixed and/or terms of similar import as used herein it meant that the metal forms, in essence, the continuous phase because the swirl formation of the deposited metal intermixes with ceramic to a degree which makes the metal dominate in the properties of the composite.
These deposits can be used as coatings or as free standing bodies. The structures can be employed in a number of specific applications. For example, they can be employed in oxidation and hot corroslon resistant materials. Further, they can be employed as thermal barriers or insulating barrier materials. Further, the structures can be employed as structural materials per se.
The metal matrix composites employing the swirl-type microstructure of the present invention are a class ofadvanced materials that hold promise for meeting a wide variety of industrial requirements. A number of potential property advantages of such structures make them particularly useful in such applications. Among these advan~ages are the , ~ ,.
~ RD-19.43 high strength to weight ratio; low density; high elastic modulus; controlled thermal expansion; and controlled thermal and electrical conduction. An important aspect of the invention is that materials can be tailored to have a desired S combination of these advantageous properties.
One of the processing techniques which is particularly suitable for the formation of structures as provided pursuant to the present invention is the low pressure plasma deposition techniques such as are taught in the patent 4,603,568. The text of the patent is incorporated herein by reference.
A distinction from the 4,603,568 teaching as carried out in the present invention is that the metal sprayed from one gun is combined instantaneously with the ceramic sprayed from the other gun in a low pressure plasma deposition chamber where both guns are aimed simultaneously at the same deposit zone of a receiving surface. ~hat was achieved by the examples recited above wa~ a simultaneous bombardment of the substrate ~ith splatters of both materials so that the two phases were interminqled and combined into a fine swirly anisotropic distribution.
The microstructure formed was deemed to have durability because of the effect of minimizing the tendency to form extensive continuous layers of ceramic. Such continuous layers of ceramic are subject to forming planes of weakness particularly during thermal cycling. The work per~ormed, as represented by Examples referred to above, demonstrated the potential of forming free standing composites and coating composites using the coordinated two gun low pressure plasma deposition processing. It was thus demonstrated that a fine interdispersion of the two material phases could be achieved and that these phases are present in a swirly intermingled microstructure. The property data obtained indicate the potential of this system for tailoring RD-l 9. a31 composite materials using the rapid solidification plasma deposition simultaneous processing of metal and ceramic materials to meet a variety of application requirements. In this regard, it has been demonstrated that density values can be lowered by combining ceramic with metal. Further, elas~ic modulus values of the composite can be increased by altering proportions of the deposited materials, and particularly by increasing the ceramic component of the composite. The overall thermal expansion coefficients of the deposit can be decreased by employing the combination of metal and ceramic materials. The control of coefficient is illustrated in the graph of Figure 6. Thermal conductivity values can be increased or decreased by judicious choice of material components for a composite system.
The use of the system makes a number of processing advantages available and these include the use of the optimal spray parameters for each of the materials. In other words, the optimal spray parameters for the metal are going to be different from the optimal spray parameters for the ceramic.
However, since the two guns are employed simultaneously but independently, the operating parameters of the guns can be adjusted to the best parameters for the material processed through that gun.
It will be understood that the invention is not limited to the employment of only two guns but that more than two guns can be employed to achieve dissimilar surprisingly advantageous structures through the development of the swirly intermixed microstructure.
Another advantage of the simultaneous two-gun processing is that the deposition angles of each material can be varied to maximize the degree to which the microstructure is intermixed and swirly and hence improved in durability.
- This is another favorable property of the deposit.
RD-14,431 A further advantage is that separate powder feeders can be used for each material to eliminate potential problem of separation due to density differences during processing when a physical mixture of two materials is used.
Claims (14)
1. The method of forming a microlaminated structure having interlaminar reinforcements which comprises, providing a first plasma gun adapted to plasma spray deposit a first material, providing a second plasma gun adapted to plasma spray deposit a second material, directing the plasma spray from both the first and second plasma guns onto the same area of a receiving surface, thereby to cause substantial swirling of the layers of deposit onto said surface and to cause thereby interlayer reinforcing strands to be formed in said deposit.
2. The method of claim 1, in which the first material is a metal.
3. The method of claim 1, in which the first and second materials are metals.
4. The method of claim 1, in which the first and second materials are metals of distinctly different properties.
5. The method of claim 1, in which the second material is a ceramic.
6. The method of claim 1, in which the first material is a metal and the second material is a ceramic.
7. The method of claim 1, in which the ratios of the materials is between 10:90 and 90:10.
RD-19,431
RD-19,431
8. The method of claim 1, in which the two materials are metals and the ratios of materials is between 10:90 and 90:10.
9. The method of claim 1, in which the ratios of materials is between 20:80 and 80:20.
10. The method of claim 1, in which the two materials are metals and the ratios of materials is between 20:80 and 80:20.
11. A microlaminated structure, said structure being made up of solidified intermixed splats of a first and of a second material, said splats having a swirly configuration whereby interlayer reinforcing strands extend from one splat to another of said structure.
12. The structure of claim 1, in which the first and second materials are metals.
13. The structure of claim 1, in which the first material is a metal and the second material is a ceramic.
14. The invention as defined in any of the preceding claims including any further features of novelty disclosed.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
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US45691989A | 1989-12-26 | 1989-12-26 | |
US456,919 | 1989-12-26 |
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CA2025302A1 true CA2025302A1 (en) | 1991-06-27 |
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CA002025302A Abandoned CA2025302A1 (en) | 1989-12-26 | 1990-09-13 | Reinforced microlaminted metal-matrix-composite structure |
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JP (1) | JPH04116149A (en) |
CA (1) | CA2025302A1 (en) |
DE (1) | DE4040893A1 (en) |
FR (1) | FR2656335A1 (en) |
GB (1) | GB2239462A (en) |
IT (1) | IT1243498B (en) |
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DE3941853C1 (en) * | 1989-12-19 | 1991-04-11 | Mtu Muenchen Gmbh | |
GB9322565D0 (en) * | 1993-11-02 | 1993-12-22 | Sprayforming Dev Ltd | Improvements in graded composites |
GB2310866A (en) * | 1996-03-05 | 1997-09-10 | Sprayforming Dev Ltd | Filling porosity or voids in articles formed by spray deposition |
DE19625274A1 (en) * | 1996-06-25 | 1998-01-02 | Lwk Plasmakeramik Gmbh & Co Kg | Mechanically reinforcing ceramic moulded parts |
EP1233081A1 (en) * | 2001-02-14 | 2002-08-21 | Siemens Aktiengesellschaft | Process and apparatus for plasma coating a turbine blade |
DE102007032804B3 (en) * | 2007-07-10 | 2008-09-04 | V&M Deutschland Gmbh | Forging mandrel for hot-forging of tubular work-pieces made of metal has a mandrel body made from heat-resistant material and a mandrel rod |
DE102007035342A1 (en) * | 2007-07-27 | 2009-01-29 | Schaeffler Kg | Method for producing a sliding layer on a plain bearing component and plain bearing component |
JP7044581B2 (en) * | 2018-02-20 | 2022-03-30 | 株式会社アルバック | Corrosion resistant membranes and vacuum parts |
BE1026683B1 (en) * | 2018-10-05 | 2020-05-07 | Soleras Advanced Coatings Bvba | SPUTTER TARGET |
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GB677144A (en) * | 1948-10-18 | 1952-08-13 | Ford Motor Co | Polymetallized light alloy brake drum |
GB680988A (en) * | 1951-07-12 | 1952-10-15 | Joseph Barry Brennan | Improvements in or relating to electrolytic devices |
FR1046251A (en) * | 1951-12-08 | 1953-12-04 | Snecma | Sintered ceramic-metal composite material which can be used in particular for the manufacture of thermal machine parts and the process for obtaining it |
GB723842A (en) * | 1951-12-08 | 1955-02-09 | Snecma | Process for the manufacture of composite metal-ceramic material |
US2920001A (en) * | 1955-07-11 | 1960-01-05 | Union Carbide Corp | Jet flame spraying method and apparatus |
SE303076B (en) * | 1963-05-15 | 1968-08-12 | Tetra Pak Ab | |
FR1600296A (en) * | 1968-12-31 | 1970-07-20 | ||
FR2148811A5 (en) * | 1971-08-04 | 1973-03-23 | Commissariat Energie Atomique | |
GB1449162A (en) * | 1973-05-25 | 1976-09-15 | Wellworthy Ltd | Method for reinforcing pistons |
JPS54103753A (en) * | 1978-02-02 | 1979-08-15 | Toyota Motor Corp | Production of aluminum-lead base alloy bearing |
US4689468A (en) * | 1986-02-10 | 1987-08-25 | Electro-Plasma, Inc. | Method of and apparatus providing oxide reduction in a plasma environment |
JPS62188769A (en) * | 1986-02-13 | 1987-08-18 | Yoshiki Tsunekawa | Manufacture of composite material by composite thermal spraying method |
JPS62188796A (en) * | 1986-02-14 | 1987-08-18 | Mazda Motor Corp | Production of fiber reinforced composite light metallic material |
US4681772A (en) * | 1986-05-05 | 1987-07-21 | General Electric Company | Method of producing extended area high quality plasma spray deposits |
US4683148A (en) * | 1986-05-05 | 1987-07-28 | General Electric Company | Method of producing high quality plasma spray deposits of complex geometry |
GB8627308D0 (en) * | 1986-11-14 | 1986-12-17 | Alcan Int Ltd | Composite metal deposit |
-
1990
- 1990-09-13 CA CA002025302A patent/CA2025302A1/en not_active Abandoned
- 1990-12-12 FR FR9015586A patent/FR2656335A1/en active Pending
- 1990-12-19 JP JP2411588A patent/JPH04116149A/en active Pending
- 1990-12-19 GB GB9027564A patent/GB2239462A/en not_active Withdrawn
- 1990-12-20 DE DE4040893A patent/DE4040893A1/en not_active Withdrawn
- 1990-12-20 IT IT02246790A patent/IT1243498B/en active IP Right Grant
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FR2656335A1 (en) | 1991-06-28 |
GB2239462A (en) | 1991-07-03 |
JPH04116149A (en) | 1992-04-16 |
IT9022467A1 (en) | 1991-06-27 |
DE4040893A1 (en) | 1991-06-27 |
IT1243498B (en) | 1994-06-15 |
GB9027564D0 (en) | 1991-02-06 |
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