fbpx
Wikipedia

Superalloy

A superalloy, or high-performance alloy, is an alloy with the ability to operate at a high fraction of its melting point.[1] Key characteristics of a superalloy include mechanical strength, thermal creep deformation resistance, surface stability, and corrosion and oxidation resistance.

Nickel superalloy jet engine (RB199) turbine blade

The crystal structure is typically face-centered cubic (FCC) austenitic. Examples of such alloys are Hastelloy, Inconel, Waspaloy, Rene alloys, Incoloy, MP98T, TMS alloys, and CMSX single crystal alloys.

Superalloy development relies on chemical and process innovations. Superalloys develop high temperature strength through solid solution strengthening and precipitation strengthening from secondary phase precipitates such as gamma prime and carbides. Oxidation or corrosion resistance is provided by elements such as aluminium and chromium. Superalloys are often cast as a single crystal in order to eliminate grain boundaries, which decrease creep resistance (even though they may provide strength at low temperatures).

The primary application for such alloys is in aerospace and marine turbine engines. Creep is typically the lifetime-limiting factor in gas turbine blades.[2]

Superalloys have made much of very-high-temperature engineering technology possible.[1]

Chemical development edit

Because these alloys are intended for high temperature applications their creep and oxidation resistance are of primary importance. Nickel (Ni)-based superalloys are the material of choice for these applications because of their unique γ' precipitates.[1][3][page needed] The properties of these superalloys can be tailored to a certain extent through the addition of various other elements, common or exotic, including not only metals, but also metalloids and nonmetals; chromium, iron, cobalt, molybdenum, tungsten, tantalum, aluminium, titanium, zirconium, niobium, rhenium, yttrium, vanadium, carbon, boron or hafnium are some examples of the alloying additions used. Each addition serves a particular purpose in optimizing properties.

Creep resistance is dependent, in part, on slowing the speed of dislocation motion within a crystal structure. In modern Ni-based superalloys, the γ'-Ni3(Al,Ti) phase acts as a barrier to dislocation. For this reason, this γ;' intermetallic phase, when present in high volume fractions, increases the strength of these alloys due to its ordered nature and high coherency with the γ matrix. The chemical additions of aluminum and titanium promote the creation of the γ' phase. The γ' phase size can be precisely controlled by careful precipitation strengthening heat treatments. Many superalloys are produced using a two-phase heat treatment that creates a dispersion of cuboidal γ' particles known as the primary phase, with a fine dispersion between these known as secondary γ'. In order to improve the oxidation resistance of these alloys, Al, Cr, B, and Y are added. The Al and Cr form oxide layers that passivate the surface and protect the superalloy from further oxidation while B and Y are used to improve the adhesion of this oxide scale to the substrate.[4] Cr, Fe, Co, Mo and Re all preferentially partition to the γ matrix while Al, Ti, Nb, Ta, and V preferentially partition to the γ' precipitates and solid solution strengthen the matrix and precipitates respectively. In addition to solid solution strengthening, if grain boundaries are present, certain elements are chosen for grain boundary strengthening. B and Zr tend to segregate to the grain boundaries which reduces the grain boundary energy and results in better grain boundary cohesion and ductility.[5] Another form of grain boundary strengthening is achieved through the addition of C and a carbide former, such as Cr, Mo, W, Nb, Ta, Ti, or Hf, which drives precipitation of carbides at grain boundaries and thereby reduces grain boundary sliding.

Ni-based superalloy compositions[1][6][7]
Element Composition range
(weight %)
Purpose
Ni, Fe, Co 50-70% These elements form the base matrix γ phase of the superalloy. Ni is necessary because it also forms γ' (Ni3Al).
Fe and Co have higher melting points than Ni and offer solid solution strengthening. Fe is also much cheaper than Ni or Co.
Cr 5-20% Cr is necessary for oxidation and corrosion resistance; it forms a protective oxide Cr2O3.
Al 0.5-6% Al is the main γ' former. It also forms a protective oxide Al2O3, which provides oxidation resistance at higher temperature than Cr2O3.
Ti 1-4% Ti forms γ'.
C 0.05-0.2% MC and M23C6 (M ⁠= ⁠metal) carbides are the strengthening phase in the absence of γ'.
B,Zr 0-0.1% Boron and zirconium provide strength to grain boundaries. This is not essential in single-crystal turbine blades, because there are no grain boundaries.
Nb 0-5% Nb can form γ'', a strengthening phase at lower (below 700 °C) temperatures.
Re, W, Hf, Mo, Ta 1-10% Refractory metals, added in small amounts for solid solution strengthening (and carbide formation). They are heavy, but have extremely high melting points.

Phase formation edit

Adding elements is usually helpful because of solid solution strengthening, but can result in unwanted precipitation. Precipitates can be classified as geometrically close-packed (GCP), topologically close-packed (TCP), or carbides. GCP phases usually benefit mechanical properties, but TCP phases are often deleterious. Because TCP phases are not truly close packed, they have few slip systems and are brittle. Also they "scavenge" elements from GCP phases. Many elements that are good for forming γ' or have great solid solution strengthening may precipitate TCPs. The proper balance promotes GCPs while avoiding TCPs.

TCP phase formation areas are weak because they:[8][9]

  • have inherently poor mechanical properties
  • are incoherent with the γ matrix
  • are surrounded by a "depletion zone" where there is no γ'
  • usually form sharp plate or needle-like morphologies which nucleate cracks

The main GCP phase is γ'. Almost all superalloys are Ni-based because of this phase. γ' is an ordered L12 (pronounced L-one-two), which means it has a certain atom on the face of the unit cell, and a certain atom on the corners of the unit cell. Ni-based superalloys usually present Ni on the faces and Ti or Al on the corners.

Another "good" GCP phase is γ''. It is also coherent with γ, but it dissolves at high temperatures.

Superalloy phases[8][9]
Phase Classification Structure Composition(s) Appearance Effect
γ matrix disordered FCC Ni, Co, Fe and other elements in solid solution The background for other precipitates The matrix phase, provides ductility and a structure for precipitates
γ' GCP L12 (ordered FCC) Ni3(Al,Ti) cubes, rounded cubes, spheres, or platelets (depending on lattice mismatch) The main strengthening phase. γ' is coherent with γ, which allows for ductility.
Carbide Carbide FCC mC, m23C6, and m6C (m ⁠= ⁠metal) string-like clumps, like strings of pearls There are many carbides, but they all provide dispersion strengthening and grain boundary stabilization.
γ'' GCP D022 (ordered BCT) Ni3Nb very small disks This precipitate is coherent with γ'. It is the main strengthening phase in IN-718, but γ'' dissolves at high temperatures.
η GCP D024 (ordered HCP) Ni3Ti may form cellular or Widmanstätten patterns The phase is not the worst, but it is not as good as γ'. It can be useful in controlling grain boundaries.
δ not close-packed orthorhombic Ni3Nb acicular (needle-like) The main issue with this phase is that it's not coherent with γ, but it is not inherently weak. It typically forms from decomposing γ'', but sometimes it's intentionally added in small amounts for grain boundary refinement.
σ TCP tetrahedral FeCr, FeCrMo, CrCo elongated globules This TCP is usually considered to have the worst mechanical properties.[10] It is never desirable for mechanical properties.
μ TCP hexagonal Fe2Nb, Co2Ti, Fe2Ti globules or platelets This phase has typical TCP issues. It is never desirable for mechanical properties.
Laves TCP rhombohedral (Fe,Co)7(Mo,W)6 coarse Widmanstätten platelets This phase has typical TCP issues. It is never desirable for mechanical properties.

Families of superalloys edit

Ni-based edit

History edit

The United States became interested in gas turbine development around 1905.[1] From 1910-1915, austenitic ( γ phase) stainless steels were developed to survive high temperatures in gas turbines. By 1929, 80Ni-20Cr alloy was the norm, with small additions of Ti and Al. Although early metallurgists did not know it yet, they were forming small γ' precipitates in Ni-based superalloys. These alloys quickly surpassed Fe- and Co-based superalloys, which were strengthened by carbides and solid solution strengthening.

Although Cr was great for protecting the alloys from oxidation and corrosion up to 700 °C, metallurgists began decreasing Cr in favor of Al, which had oxidation resistance at much higher temperatures. The lack of Cr caused issues with hot corrosion, so coatings needed to be developed.

Around 1950, vacuum melting became commercialized, which allowed metallurgists to create higher purity alloys with more precise composition.

In the 60s and 70s, metallurgists changed focus from alloy chemistry to alloy processing. Directional solidification was developed to allow columnar or even single-crystal turbine blades. Oxide dispersion strengthening could obtain very fine grains and superplasticity.

Phases edit

  • Gamma (γ): This phase composes the matrix of Ni-based superalloy. It is a solid solution fcc austenitic phase of the alloying elements.[10][11] The alloying elements most found in commercial Ni-based alloys are, C, Cr, Mo, W, Nb, Fe, Ti, Al, V, and Ta. During the formation of these materials, as they cool from the melt, carbides precipitate, and at even lower temperatures γ' phase precipitates.[11][12]
  • Gamma prime (γ'): This phase constitutes the precipitate used to strengthen the alloy. It is an intermetallic phase based on Ni3(Ti,Al) which have an ordered FCC L12 structure.[10] The γ' phase is coherent with the matrix of the superalloy having a lattice parameter that varies by around 0.5%. Ni3(Ti,Al) are ordered systems with Ni atoms at the cube faces and either Al or Ti atoms at the cube edges. As particles of γ' precipitates aggregate, they decrease their energy states by aligning along the <100> directions forming cuboidal structures.[11] This phase has a window of instability between 600 °C and 850 °C, inside of which γ' will transform into the HCP η phase. For applications at temperatures below 650 °C, the γ" phase can be utilized for strengthening.[13]
 
Crystal structure for γ" (Ni3Nb) (Body Centered Tetragonal)
  • Gamma double prime (γ"): This phase typically is Ni3Nb or Ni3V and is used to strengthen Ni-based superalloys at lower temperatures (<650 °C) relative to γ'. The crystal structure of γ" is body-centered tetragonal (BCT), and the phase precipitates as 60 nm by 10 nm discs with the (001) planes in γ" parallel to the {001} family in γ. These anisotropic discs form as a result of lattice mismatch between the BCT precipitate and the FCC matrix. This lattice mismatch leads to high coherency strains which, together with order hardening, are the primary strengthening mechanisms. The γ" phase is unstable above approximately 650 °C.[13]
  • Carbide phases: Carbide formation is usually deleterious although in Ni-based superalloys they are used to stabilize the structure of the material against deformation at high temperatures. Carbides form at the grain boundaries, inhibiting grain boundary motion.[10][11]
  • Topologically close-packed (TCP) phases: The term "TCP phase" refers to any member of a family of phases (including the σ phase, the χ phase, the μ phase, and the Laves phase), which are not atomically close-packed but possess some close-packed planes with HCP stacking. TCP phases tend to be highly brittle and deplete the γ matrix of strengthening, solid solution refractory elements (including Cr, Co, W, and Mo). These phases form as a result of kinetics after long periods of time (thousands of hours) at high temperatures (>750 °C).[13]

Co-based edit

Co-based superalloys depend on carbide precipitation and solid solution strengthening for mechanical properties. While these strengthening mechanisms are inferior to gamma prime (γ') precipitation strengthening,[1] cobalt has a higher melting point than nickel and has superior hot corrosion resistance and thermal fatigue. As a result, carbide-strengthened Co-based superalloys are used in lower stress, higher temperature applications such as stationary vanes in gas turbines.[14]

Co's γ/γ' microstructure was rediscovered and published in 2006 by Sato et al.[15] That γ' phase was Co3(Al, W). Mo, Ti, Nb, V, and Ta partition to the γ' phase, while Fe, Mn, and Cr partition to the matrix γ.

The next family of Co-based superalloys was discovered in 2015 by Makineni et al. This family has a similar γ/γ' microstructure, but is W-free and has a γ' phase of Co3(Al,Mo,Nb).[16] Since W is heavy, its elimination makes Co-based alloys increasingly viable in turbines for aircraft, where low density is especially valued.

The most recently discovered family of superalloys was computationally predicted by Nyshadham et al. in 2017,[17] and demonstrated by Reyes Tirado et al. in 2018.[18] This γ' phase is W free and has the composition Co3(Nb,V) and Co3(Ta,V).

Phases edit

  • Gamma (γ): This is the matrix phase. While Co-based superalloys are less-used commercially, alloying elements include C, Cr, W, Ni, Ti, Al, Ir, and Ta.[15][19] As in stainless steels, Chromium is used (occasionally up to 20 wt.%) to improve resistance to oxidation and corrosion via the formation of a Cr2O3 passive layer, which is critical for use in gas turbines, but also provides solid-solution strengthening due to the mismatch in the atomic radii of Co and Cr, and precipitation hardening due to the formation of MC-type carbides.[20]
  • Gamma Prime (γ'): Constitutes the precipitate used to strengthen the alloy. It is usually close-packed with a L12 structure of Co3Ti or FCC Co3Ta, though both W and Al integrate into these cuboidal precipitates. Ta, Nb, and Ti integrate into the γ' phase and are stabilize it at high temperatures. [15][21]
  • Carbide Phases: Carbides strengthen the alloy through precipitation hardening but decrease low-temperature ductility.[19]
  • Topologically Close-Packed (TCP) phases may appear in some Co-based superalloys, but embrittle the alloy and are thus undesirable.

Fe-based edit

Steel superalloys are of interest because some present creep and oxidation resistance similar to Ni-based superalloys, at far less cost.

Gamma (γ): Fe-based alloys feature a matrix phase of austenite iron (FCC). Alloying elements include: Al, B, C, Co, Cr, Mo, Ni, Nb, Si, Ti, W, and Y.[22] Al (oxidation benefits) must be kept at low weight fractions (wt.%) because Al stabilizes a ferritic (BCC) primary phase matrix, which is undesirable, as it is inferior to the high temperature strength exhibited by an austenitic (FCC) primary phase matrix.[23]

Gamma-prime (γ'): This phase is introduced as precipitates to strengthen the alloy. γ'-Ni3Al precipitates can be introduced with the proper balance of Al, Ni, Nb, and Ti additions.

Microstructure edit

The two major types of austenitic stainless steels are characterized by the oxide layer that forms on the steel surface: either chromia-forming or alumina-forming. Cr-forming stainless steel is the most common type. However, Cr-forming steels do not exhibit high creep resistance at high temperatures, especially in environments with water vapor. Exposure to water vapor at high temperatures can increase internal oxidation in Cr-forming alloys and rapid formation of volatile Cr (oxy)hydroxides, both of which can reduce durability and lifetime.[23]

Al-forming austenitic stainless steels feature a single-phase matrix of austenite iron (FCC) with an Al-oxide at the surface of the steel. Al is more thermodynamically stable in oxygen than Cr. More commonly, however, precipitate phases are introduced to increase strength and creep resistance. In Al-forming steels, NiAl precipitates are introduced to act as Al reservoirs to maintain the protective alumina layer. In addition, Nb and Cr additions help form and stabilize Al by increasing precipitate volume fractions of NiAl.[23]

At least 5 grades of alumina-forming austenitic (AFA) alloys, with different operating temperatures at oxidation in air + 10% water vapor have been realized:[24]

  • AFA Grade: (50-60)Fe-(20-25)Ni-(14-15)Cr-(2.5-3.5)Al-(1-3)Nb wt.% base
    • 750-800 °C operating temperatures at oxidation in air + 10% water vapor
  • Low Nickel AFA Grade: 63Fe-12Ni-14Cr-2.5Al-0.6Nb-5Mn3Cu wt.% base
    • 650 °C operating temperatures at oxidation in air + 10% water vapor
  • High Performance AFA Grade: (45-55)Fe-(25-30)Ni-(14-15)Cr(3.5-4.5)Al-(1-3)Nb-(0.02-0.1)Hf/Y wt.% base
    • 850-900 °C operating temperatures at oxidation in air + 10% water vapor
  • Cast AFA Grade: (35-50)Fe-(25-35)Ni-14Cr-(3.5-4)Al-1Nb wt.% base
    • 750-1100 °C operating temperatures at oxidation in air + 10% water vapor, depending upon Ni wt.%
  • AFA superalloy (40-50)Fe-(30-35)Ni-(14-19)Cr-(2.5-3.5)Al-3Nb
    • 750-850 °C operating temperatures at oxidation in air + 10% water vapor

Operating temperatures with oxidation in air and no water vapor are expected to be higher. In addition, an AFA superalloy grade exhibits creep strength approaching that of nickel alloy UNS N06617.

Microstructure edit

In pure Ni3Al phase Al atoms are placed at the vertices of the cubic cell and form sublattice A. Ni atoms are located at centers of the faces and form sublattice B. The phase is not strictly stoichiometric. An excess of vacancies in one of the sublattices may exist, which leads to deviations from stoichiometry. Sublattices A and B of the γ' phase can solute a considerable proportion of other elements. The alloying elements are dissolved in the γ phase. The γ' phase hardens the alloy through the yield strength anomaly. Dislocations dissociate in the γ' phase, leading to the formation of an anti-phase boundary. At elevated temperature, the free energy associated with the anti-phase boundary (APB) is considerably reduced if it lies on a particular plane, which by coincidence is not a permitted slip plane. One set of partial dislocations bounding the APB cross-slips so that the APB lies on the low-energy plane, and, since this low-energy plane is not a permitted slip plane, the dissociated dislocation is effectively locked. By this mechanism, the yield strength of γ' phase Ni3Al increases with temperature up to about 1000 °C.

Initial material selection for blade applications in gas turbine engines included alloys like the Nimonic series alloys in the 1940s.[3][page needed] The early Nimonic series incorporated γ' Ni3(Al,Ti) precipitates in a γ matrix, as well as various metal-carbon carbides (e.g. Cr23C6) at the grain boundaries[25] for additional grain boundary strength. Turbine blade components were forged until vacuum induction casting technologies were introduced in the 1950s.[3][page needed] This process significantly improved cleanliness, reduced defects, and increased the strength and temperature capability.

Modern superalloys were developed in the 1980s. First generation superalloys incorporated increased Al, Ti, Ta, and Nb content in order to increase the γ' volume fraction. Examples include: PWA1480, René N4 and SRR99. Additionally, the volume fraction of the γ' precipitates increased to about 50–70% with the advent of monocrystal solidification techniques that enable grain boundaries to be entirely eliminated. Because the material contains no grain boundaries, carbides are unnecessary as grain boundary strengthers and were thus eliminated.[3][page needed]

Second and third generation superalloys introduce about 3 and 6 weight percent rhenium, for increased temperature capability. Re is a slow diffuser and typically partitions the γ matrix, decreasing the rate of diffusion (and thereby high temperature creep) and improving high temperature performance and increasing service temperatures by 30 °C and 60 °C in second and third generation superalloys, respectively.[26] Re promotes the formation of rafts of the γ' phase (as opposed to cuboidal precipitates). The presence of rafts can decrease creep rate in the power-law regime (controlled by dislocation climb), but can also potentially increase the creep rate if the dominant mechanism is particle shearing. Re tends to promote the formation of brittle TCP phases, which has led to the strategy of reducing Co, W, Mo, and particularly Cr. Later generations of Ni-based superalloys significantly reduced Cr content for this reason, however with the reduction in Cr comes a reduction in oxidation resistance. Advanced coating techniques offset the loss of oxidation resistance accompanying the decreased Cr contents.[13][27] Examples of second generation superalloys include PWA1484, CMSX-4 and René N5.

Third generation alloys include CMSX-10, and René N6. Fourth, fifth, and sixth generation superalloys incorporate ruthenium additions, making them more expensive than prior Re-containing alloys. The effect of Ru on the promotion of TCP phases is not well-determined. Early reports claimed that Ru decreased the supersaturation of Re in the matrix and thereby diminished the susceptibility to TCP phase formation.[28] Later studies noted an opposite effect. Chen, et al., found that in two alloys differing significantly only in Ru content (USTB-F3 and USTB-F6) that the addition of Ru increased both the partitioning ratio as well as supersaturation in the γ matrix of Cr and Re, and thereby promoted the formation of TCP phases.[29]

The current trend is to avoid very expensive and very heavy elements. An example is Eglin steel, a budget material with compromised temperature range and chemical resistance. It does not contain rhenium or ruthenium and its nickel content is limited. To reduce fabrication costs, it was chemically designed to melt in a ladle (though with improved properties in a vacuum crucible). Conventional welding and casting is possible before heat-treatment. The original purpose was to produce high-performance, inexpensive bomb casings, but the material has proven widely applicable to structural applications, including armor.

Single-crystal superalloys edit

Single-crystal superalloys (SX or SC superalloys) are formed as a single crystal using a modified version of the directional solidification technique, leaving no grain boundaries. The mechanical properties of most other alloys depend on the presence of grain boundaries, but at high temperatures, they participate in creep and require other mechanisms. In many such alloys, islands of an ordered intermetallic phase sit in a matrix of disordered phase, all with the same crystal lattice. This approximates the dislocation-pinning behavior of grain boundaries, without introducing any amorphous solid into the structure.

Single crystal (SX) superalloys have wide application in the high-pressure turbine section of aero- and industrial gas turbine engines due to the unique combination of properties and performance. Since introduction of single crystal casting technology, SX alloy development has focused on increased temperature capability, and major improvements in alloy performance are associated with rhenium (Re) and ruthenium (Ru).[30]

The creep deformation behavior of superalloy single crystal is strongly temperature-, stress-, orientation- and alloy-dependent. For a single-crystal superalloy, three modes of creep deformation occur under regimes of different temperature and stress: rafting, tertiary, and primary.[31][page needed] At low temperature (~750 °C), SX alloys exhibits mostly primary creep behavior. Matan et al. concluded that the extent of primary creep deformation depends strongly on the angle between the tensile axis and the <001>/<011> symmetry boundary.[32] At temperatures above 850 °C, tertiary creep dominates and promotes strain softening behavior.[3][page needed] When temperature exceeds 1000 °C, the rafting effect is prevalent where cubic particles transform into flat shapes under tensile stress.[33] The rafts form perpendicular to the tensile axis, since γ phase is transported out of the vertical channels and into the horizontal ones. Reed et al. studied unaxial creep deformation of <001> oriented CMSX-4 single crystal superalloy at 1105 °C and 100 MPa. They reported that rafting is beneficial to creep life since it delays evolution of creep strain. In addition, rafting occurs quickly and suppresses the accumulation of creep strain until a critical strain is reached.[34]

Oxidation edit

For superalloys operating at high temperatures and exposed to corrosive environments, oxidation behavior is a concern. Oxidation involves chemical reactions of the alloying elements with oxygen to form new oxide phases, generally at the alloy surface. If unmitigated, oxidation can degrade the alloy over time in a variety of ways, including:[35][36]

  • sequential surface oxidation, cracking, and spalling, eroding the alloy over time
  • surface embrittlement through the introduction of oxide phases, promoting crack formation and fatigue failure
  • depletion of key alloying elements, affecting mechanical properties and possibly compromising performance

Selective oxidation is the primary strategy used to limit these deleterious processes. The ratio of alloying elements promotes formation of a specific oxide phase that then acts as a barrier to further oxidation. Most commonly, aluminum and chromium are used in this role, because they form relatively thin and continuous oxide layers of alumina (Al2O3) and chromia (Cr2O3), respectively. They offer low oxygen diffusivities, effectively halting further oxidation beneath this layer. In the ideal case, oxidation proceeds through two stages. First, transient oxidation involves the conversion of various elements, especially the majority elements (e.g. nickel or cobalt). Transient oxidation proceeds until the selective oxidation of the sacrificial element forms a complete barrier layer.[35]

The protective effect of selective oxidation can be undermined. The continuity of the oxide layer can be compromised by mechanical disruption due to stress or may be disrupted as a result of oxidation kinetics (e.g. if oxygen diffuses too quickly). If the layer is not continuous, its effectiveness as a diffusion barrier to oxygen is compromised. The stability of the oxide layer is strongly influenced by the presence of other minority elements. For example, the addition of boron, silicon, and yttrium to superalloys promotes oxide layer adhesion, reducing spalling and maintaining continuity.[37]

Oxidation is the most basic form of chemical degradation superalloys may experience. More complex corrosion processes are common when operating environments include salts and sulfur compounds, or under chemical conditions that change dramatically over time. These issues are also often addressed through comparable coatings.

Processing edit

Superalloys were originally iron-based and cold wrought prior to the 1940s when investment casting of cobalt base alloys significantly raised operating temperatures. The 1950s development of vacuum melting allowed for fine control of the chemical composition of superalloys and reduction in contamination and in turn led to a revolution in processing techniques such as directional solidification of alloys and single crystal superalloys.[38][page needed]

Processing methods vary widely depending on the required properties of each item.

Casting and forging edit

Casting and forging are traditional metallurgical processing techniques that can be used to generate both polycrystalline and monocrystalline products. Polycrystalline casts offer higher fracture resistance, while monocrystalline casts offer higher creep resistance.

Jet turbine engines employ both crystalline component types to take advantage of their individual strengths. The disks of the high-pressure turbine, which are near the central hub of the engine are polycrystalline. The turbine blades, which extend radially into the engine housing, experience a much greater centripetal force, necessitating creep resistance, typically adopting monocrystalline or polycrystalline with a preferred crystal orientation.

Investment casting edit

Investment casting is a metallurgical processing technique in which a wax form is fabricated and used as a template for a ceramic mold. A ceramic mold is poured around the wax form and solidifies, the wax form is melted out of the ceramic mold, and molten metal is poured into the void left by the wax. This leads to a metal form in the same shape as the original wax form. Investment casting leads to a polycrystalline final product, as nucleation and growth of crystal grains occurs at numerous locations throughout the solid matrix. Generally, the polycrystalline product has no preferred grain orientation.

Directional solidification edit

 
Schematic of directional solidification

Directional solidification uses a thermal gradient to promote nucleation of metal grains on a low temperature surface, as well as to promote their growth along the temperature gradient. This leads to grains elongated along the temperature gradient, and significantly greater creep resistance parallel to the long grain direction. In polycrystalline turbine blades, directional solidification is used to orient the grains parallel to the centripetal force. It is also known as dendritic solidification.

Single crystal growth edit

Single crystal growth starts with a seed crystal that is used to template growth of a larger crystal. The overall process is lengthy, and machining is necessary after the single crystal is grown.

Powder metallurgy edit

Powder metallurgy is a class of modern processing techniques in which metals are first powdered, and then formed into the desired shape by heating below the melting point. This is in contrast to casting, which occurs with molten metal. Superalloy manufacturing often employs powder metallurgy because of its material efficiency - typically much less waste metal must be machined away from the final product—and its ability to facilitate mechanical alloying. Mechanical alloying is a process by which reinforcing particles are incorporated into the superalloy matrix material by repeated fracture and welding.[39][failed verification]

Sintering and hot isostatic pressing edit

Sintering and hot isostatic pressing are processing techniques used to densify materials from a loosely packed "green body" into a solid object with physically merged grains. Sintering occurs below the melting point, and causes adjacent particles to merge at their boundaries, creating a strong bond between them. In hot isostatic pressing, a sintered material is placed in a pressure vessel and compressed from all directions (isostatically) in an inert atmosphere to affect densification.[40]

Additive manufacturing edit

Selective laser melting (also known as powder bed fusion) is an additive manufacturing procedure used to create intricately detailed forms from a CAD file. A shape is designed and then converted into slices. These slices are sent to a laser writer to print the final product. In brief, a bed of metal powder is prepared, and a slice is formed in the powder bed by a high energy laser sintering the particles together. The powder bed moves downwards, and a new batch of metal powder is rolled over the top. This layer is then sintered with the laser, and the process is repeated until all slices have been processed.[41] Additive manufacturing can leave pores behind. Many products undergo a heat treatment or hot isostatic pressing procedure to densify the product and reduce porosity.[42]

Coatings edit

In modern gas turbines, the turbine entry temperature (~1750K) exceeds superalloy incipient melting temperature (~1600K), with the help of surface engineering.[43][page needed]

Types edit

The three types of coatings are: diffusion coatings, overlay coatings, and thermal barrier coatings. Diffusion coatings, mainly constituted with aluminide or platinum-aluminide, is the most common. MCrAlX-based overlay coatings (M=Ni or Co, X=Y, Hf, Si) enhance resistance to corrosion and oxidation. Compared to diffusion coatings, overlay coatings are more expensive, but less dependent on substrate composition, since they must be carried out by air or vacuum plasma spraying (APS/VPS)[44][page needed] or electron beam physical vapour deposition (EB-PVD).[45] Thermal barrier coatings provide by far the best enhancement in working temperature and coating life. It is estimated that modern TBC of thickness 300 μm, if used in conjunction with a hollow component and cooling air, has the potential to lower metal surface temperatures by a few hundred degrees.[46]

Thermal barrier coatings edit

Thermal barrier coatings (TBCs) are used extensively in gas turbine engines to increase component life and engine performance.[47] A coating of about 1-200 µm can reduce the temperature at the superalloy surface by up to 200 K. TBCs are a system of coatings consisting of a bond coat, a thermally grown oxide (TGO), and a thermally insulating ceramic top coat. In most applications, the bond coat is either a MCrAlY (where M=Ni or NiCo) or a Pt modified aluminide coating. A dense bond coat is required to provide protection of the superalloy substrate from oxidation and hot corrosion attack and to form an adherent, slow-growing surface TGO. The TGO is formed by oxidation of the aluminum that is contained in the bond coat. The current (first generation) thermal insulation layer is composed of 7wt % yttria-stabilized zirconia (7YSZ) with a typical thickness of 100–300 µm. Yttria-stabilized zirconia is used due to its low thermal conductivity (2.6W/mK for fully dense material), relatively high coefficient of thermal expansion, and high temperature stability. The electron beam-directed vapor deposition (EB-DVD) process used to apply the TBC to turbine airfoils produces a columnar microstructure with multiple porosity levels. Inter-column porosity is critical to providing strain tolerance (via a low in-plane modulus), as it would otherwise spall on thermal cycling due to thermal expansion mismatch with the superalloy substrate. This porosity reduces the thermal coating's conductivity.

Bond coat edit

The bond coat adheres the thermal barrier to the substrate. Additionally, the bond coat provides oxidation protection and functions as a diffusion barrier against the motion of substrate atoms towards the environment. The five major types of bond coats are: the aluminides, the platinum-aluminides, MCrAlY, cobalt-cermets, and nickel-chromium. For aluminide bond coatings, the coating's final composition and structure depends on the substrate composition. Aluminides lack ductility below 750 °C, and exhibit limited thermomechanical fatigue strength. Pt-aluminides are similar to the aluminide bond coats except for a layer of Pt (5—10 μm) deposited on the blade. The Pt aids in oxide adhesion and contributes to hot corrosion, increasing blade lifespan. MCrAlY does not strongly interact with the substrate. Normally applied by plasma spraying, MCrAlY coatings from secondary aluminum oxides. This means that the coatings form an outer chromia layer and a secondary alumina layer underneath. These oxide formations occur at high temperatures in the range of those that superalloys usually encounter.[48] The chromia provides oxidation and hot-corrosion resistance. The alumina controls oxidation mechanisms by limiting oxide growth by self-passivating. The yttrium enhances oxide adherence to the substrate, and limits the growth of grain boundaries (which can lead to coat flaking).[49] Addition of rhenium and tantalum increases oxidation resistance. Cobalt-cermet-based coatings consisting of materials such as tungsten carbide/cobalt can be used due to excellent resistance to abrasion, corrosion, erosion, and heat.[50][full citation needed] These cermet coatings perform well in situations where temperature and oxidation damage are significant concerns, such as boilers. One of cobalt cermet's unique advantages is minimal loss of coating mass over time, due to the strength of carbides. Overall, cermet coatings are useful in situations where mechanical demands are equal to chemical demands. Nickel-chromium coatings are used most frequently in boilers fed by fossil fuels, electric furnaces, and waste incineration furnaces, where the danger of oxidizing agents and corrosive compounds in the vapor must be addressed.[51] The specific method of spray-coating depends on the coating composition. Nickel-chromium coatings that also contain iron or aluminum provide better corrosion resistance when they are sprayed and laser glazed, while pure nickel-chromium coatings perform better when thermally sprayed exclusively.[52]

Process methods edit

Several kinds of coating process are available: pack cementation process, gas phase coating (both are a type of chemical vapor deposition (CVD)), thermal spraying, and physical vapor deposition. In most cases, after the coating process, near-surface regions of parts are enriched with aluminium in a matrix of the nickel aluminide.

Pack cementation edit

Pack cementation is a widely used CVD technique that consists of immersing the components to be coated in a metal powder mixture and ammonium halide activators and sealing them in a retort. The entire apparatus is placed inside a furnace and heated in a protective atmosphere to a lower than normal temperature that allows diffusion, due to the halide salts chemical reaction that causes a eutectic bond between the two metals. The surface alloy that is formed due to thermal-diffused ion migration has a metallurgical bond to the substrate and an intermetallic layer found in the gamma layer of the surface alloys.

The traditional pack consists of four components at temperatures below (750 °C):

  • Substrate or parts
  • Ferrous and non-ferrous powdered alloy: (Ti and/or Al, Si and/or Zn, B and/ or Cr)
  • Halide salt activator: Ammonium halide salts
  • Relatively inert filler powder (Al2O3, SiO2, or SiC)

This process includes:

  • Aluminizing
  • Chromizing
  • Siliconizing
  • Sherardizing
  • Boronizing
  • Titaniumizing

Pack cementation has reemerged when combined with other chemical processes to lower the temperatures of metal combinations and give intermetallic properties to different alloy combinations for surface treatments.

Thermal spraying edit

Thermal spraying involves heating a feedstock of precursor material and spraying it on a surface. Specific techniques depend on desired particle size, coat thickness, spray speed, desired area, etc.[53][full citation needed] Thermal spraying relies on adhesion to the surface. As a result, the surface of the superalloy must be cleaned and prepared, and usually polished, before application.[54]

Plasma spraying edit

Plasma spraying offers versatility of usable coatings, and high-temperature performance.[55] Plasma spraying can accommodate a wide range of materials, versus other techniques. As long as the difference between melting and decomposition temperatures is greater than 300 K, plasma spraying is viable.[56][page needed]

Gas phase edit

Gas phase coating is carried out at higher temperatures, about 1080 °C. The coating material is usually loaded onto trays without physical contact with the parts to be coated. The coating mixture contains active coating material and activator, but usually not thermal ballast. As in the pack cementation process, gaseous aluminium chloride (or fluoride) is transferred to the surface of the part. However, in this case the diffusion is outwards. This kind of coating also requires diffusion heat treatment.

Failure mechanisms edit

Failure of thermal barrier coating usually manifests as delamination, which arises from the temperature gradient during thermal cycling between ambient temperature and working conditions coupled with the difference in thermal expansion coefficient of substrate and coating. It is rare for the coating to fail completely – some pieces remain intact, and significant scatter is observed in the time to failure if testing is repeated under identical conditions.[3][page needed] Various degradation mechanisms affect thermal barrier coating,[57][58] and some or all of these must operate before failure finally occurs:

  • Oxidation at the interface of thermal barrier coating and underlying bond coat;[59]
  • Depletion of aluminum in bond coat due to oxidation[60] and diffusion with substrate;[61]
  • Thermal stresses from mismatch in thermal expansion coefficient and growth stress due to the formation of thermally grown oxide layer;[62]
  • Imperfections near thermally grown oxide layer;[63][64][65]
  • Various other complicating factors during engine operation.[66][67][68][69][70]

Additionally, TBC life is sensitive to the combination of materials (substrate, bond coat, ceramic) and processes (EB-PVD, plasma spraying) used.

Applications edit

Turbines edit

Nickel-based superalloys are used in load-bearing structures requiring the highest homologous temperature of any common alloy system (Tm = 0.9, or 90% of their melting point). Among the most demanding applications for a structural material are those in the hot sections of turbine engines (e.g. turbine blade). They comprise over 50% of the weight of advanced aircraft engines. The widespread use of superalloys in turbine engines coupled with the fact that the thermodynamic efficiency of turbine engines is a function of increasing turbine inlet temperatures has provided part of the motivation for increasing the maximum-use temperature of superalloys. From 1990-2020, turbine airfoil temperature capability increased on average by about 2.2 °C/year. Two major factors have made this increase possible:[citation needed]

  • Processing techniques that improved alloy cleanliness (thus improving reliability) and/or enabled the production of tailored microstructures such as directionally solidified or single-crystal material.
  • Alloy development resulting in higher temperature materials primarily through the additions of refractory elements such as Re, W, Ta, and Mo.

About 60% of the temperature increases related to advanced cooling, while 40% have resulted from material improvements. State-of-the-art turbine blade surface temperatures approach 1,150 C. The most severe stress and temperature combinations correspond to an average bulk metal temperature approaching 1,000 C..

Although Ni-based superalloys retain significant strength to 980 C, they tend to be susceptible to environmental attack because of the presence of reactive alloying elements. Surface attack includes oxidation, hot corrosion, and thermal fatigue.[10]

Energy production edit

High temperature materials are valuable for energy conversion and energy production applications. Maximum energy conversion efficiency is desired in such applications, in accord with the Carnot cycle. Because Carnot efficiency is limited by the temperature difference between the hot and cold reservoirs, higher operating temperatures increase energy conversion efficiency. Operating temperatures are limited by superalloys, limiting applications to around 1000 °C-1400 °C. Energy applications include:[71]

  • Solar thermal power plants (stainless steel rods containing heated water)
  • Steam turbines (turbine blades and boiler housing)
  • Heat exchangers for nuclear reactor systems

Alumina-forming stainless steel is weldable and has potential for use in automotive applications, such as for high temperature exhaust piping and in heat capture and reuse.

Research edit

Radiolysis edit

Sandia National Laboratories is studying radiolysis for making superalloys. It uses nanoparticle synthesis to create alloys and superalloys. This process holds promise as a universal method of nanoparticle formation. By developing an understanding of the basic material science, it might be possible to expand research into other aspects of superalloys. Radiolysis produces polycrystalline alloys, which suffer from an unacceptable level of creep.

Austentic steel edit

Stainless steel alloys remain a research target because of lower production costs, as well as the need for an austenitic stainless steel with high-temperature corrosion resistance in environments with water vapor. Research focuses on increasing high-temperature tensile strength, toughness, and creep resistance to compete with Ni-based superalloys.[24]

Oak Ridge National Laboratory is researching austentic alloys, achieving similar creep and corrosion resistance at 800 °C to that of other austenitic alloys, including Ni-based superalloys.[24]

AFA superalloys edit

Development of AFA superalloys with a 35 wt.% Ni-base have shown potential for use in operating temperatures upwards to 1,100 °C.[24]

Multi-principal-element superalloy (MPES) edit

Researchers at Sandia Labs, Ames National Laboratory and Iowa State University reported a 3D-printed superalloy composed of 42% aluminum, 25% titanium, 13% niobium, 8% zirconium, 8% molybdenum and 4% tantalum. Most alloys are made chiefly of one primary element, combined with low amounts of other elements. In contrast MPES have substantial amounts of three or more elements.[72]

Such alloys promise improvements on high-temperature applications, strength-to-weight, fracture toughness, corrosion and radiation resistance, wear resistance, and others. They reported hardness and density of 1.8–2.6 GPa-cm3/g, which surpasses all known alloys, including intermetallic compounds, titanium aluminides, refractory MPEAs, and conventional Ni-based superalloys. This represents a 300% improvement over Inconel 718 based on measured peak hardness of 4.5 GPa and density of 8.2 g/cm3, (0.55 GPa-cm3/g).[72]

The material is stable at 800 °C, hotter than the 570+ °C found in typical coal-based power plants.[72]

The researchers acknowedged that the 3D printing process produces microscopic cracks when forming large parts, and that the feedstock includes metals that limit applicability in cost-sensitive applications.[72]

See also edit

References edit

  1. ^ a b c d e f Sims, C.T. (1984). "A History of Superalloy Metallurgy for Superalloy Metallurgists". Superalloys 1984 (Fifth International Symposium). pp. 399–419. doi:10.7449/1984/Superalloys_1984_399_419.
  2. ^ Carter, Tim J (April 2005). "Common failures in gas turbine blades". Engineering Failure Analysis. 12 (2): 237–247. doi:10.1016/j.engfailanal.2004.07.004.
  3. ^ a b c d e f Reed, R. C (2008). The Superalloys: Fundamentals and Applications. Cambridge: Cambridge University Press. ISBN 9780521070119.
  4. ^ Klein, L.; Shen, Y.; Killian, M. S.; Virtanen, S. (2011). "Effect of B and Cr on the high temperature oxidation behaviour of novel γ/γ'-strengthened Co-base superalloys". Corrosion Science. 53 (9): 2713–720. doi:10.1016/j.corsci.2011.04.020.
  5. ^ Shinagawa, K.; Omori, Toshihiro; Oikawa, Katsunari; Kainuma, Ryosuke; Ishida, Kiyohito (2009). "Ductility Enhancement by Boron Addition in Co–Al–W High-temperature Alloys". Scripta Materialia. 61 (6): 612–15. doi:10.1016/j.scriptamat.2009.05.037.
  6. ^ Giamei, Anthony (September 2013). "Development of Single Crystal Superalloys: A Brief History". Advanced Materials & Processes: 26–30 – via asminternational.
  7. ^ Akca, Enes; Gursel, Ali (2015). "A Review on Superalloys and IN718 Nickel-Based INCONEL Superalloy". Periodicals of Engineering and Natural Sciences. 3 (1): 15–27. doi:10.21533/pen.v3i1.43 – via pen.ius.edu.ba.
  8. ^ a b Belan, Juraj (2016). "GCP and TCP Phases Presented in Nickel-base Superalloys". Materials Today: Proceedings. 3 (4): 936–941. doi:10.1016/j.matpr.2016.03.024.
  9. ^ a b Rae, C.M.F.; Karunaratne, M.S.A.; Small, C.J.; Broomfield, R.W.; Jones, C.N.; Reed, R.C. (2000). "Topologically Close Packed Phases in an Experimental Rhenium-Containing Single Crystal Superalloy". Superalloys 2000 (Ninth International Symposium). pp. 767–776. doi:10.7449/2000/Superalloys_2000_767_776. ISBN 0-87339-477-1.
  10. ^ a b c d e Randy Bowman. "Superalloys: A Primer and History". Retrieved 6 March 2020 – via tms.org.
  11. ^ a b c d Sabol, G. P.; Stickler, R. (1969). "Microstructure of Nickel-Based Superalloys". Physica Status Solidi B. 35 (1): 11–52. Bibcode:1969PSSBR..35...11S. doi:10.1002/pssb.19690350102.
  12. ^ Doi, M.; Miki, D.; Moritani, T.; Kozakai, T. (2004). "Gamma/Gamma-Prime Microstructure Formed by Phased Separation of Gamma-Prime Precipitates in a Ni-Al-Ti Alloy". Superalloys 2004 (Tenth International Symposium). pp. 109–114. doi:10.7449/2004/Superalloys_2004_109_114. ISBN 0-87339-576-X.
  13. ^ a b c d Dunand, David C. "Materials Science & Engineering 435: High Temperature Materials". Northwestern University, Evanston. 25 February 2016. Lecture.
  14. ^ Institute, Cobalt (14 February 2018). "Superalloys". www.cobaltinstitute.org. Retrieved 10 December 2019.
  15. ^ a b c Sato, J (2006). "Cobalt-Base High-Temperature Alloys". Science. 312 (5770): 90–91. Bibcode:2006Sci...312...90S. doi:10.1126/science.1121738. PMID 16601187. S2CID 23877638.
  16. ^ Makineni, S. K.; Nithin, B.; Chattopadhyay, K. (March 2015). "A new tungsten-free γ–γ' Co–Al–Mo–Nb-based superalloy". Scripta Materialia. 98: 36–39. doi:10.1016/j.scriptamat.2014.11.009.
  17. ^ Nyshadham, Chandramouli; Oses, Corey; Hansen, Jacob E.; Takeuchi, Ichiro; Curtarolo, Stefano; Hart, Gus L.W. (January 2017). "A computational high-throughput search for new ternary superalloys". Acta Materialia. 122: 438–447. arXiv:1603.05967. Bibcode:2017AcMat.122..438N. doi:10.1016/j.actamat.2016.09.017. S2CID 11222811.
  18. ^ Reyes Tirado, Fernando L.; Perrin Toinin, Jacques; Dunand, David C. (June 2018). "γ+γ' microstructures in the Co-Ta-V and Co-Nb-V ternary systems". Acta Materialia. 151: 137–148. doi:10.1016/j.actamat.2018.03.057.
  19. ^ a b Cui, C (2006). "A New Co-Base Superalloy Strengthened by γ' Phase". Materials Transactions. 47 (8): 2099–2102. doi:10.2320/matertrans.47.2099.
  20. ^ Coutsouradis, D.; Davin, A.; Lamberigts, M. (April 1987). "Cobalt-based superalloys for applications in gas turbines". Materials Science and Engineering. 88: 11–19. doi:10.1016/0025-5416(87)90061-9.
  21. ^ Suzuki, A.; Pollock, Tresa M. (2008). "High-temperature strength and deformation of γ/γ' two-phase Co–Al–W-base alloys". Acta Materialia. 56 (6): 1288–97. doi:10.1016/j.actamat.2007.11.014.
  22. ^ "Review: precipitation in austenitic stainless steels". www.phase-trans.msm.cam.ac.uk. Retrieved 2 March 2018.
  23. ^ a b c Brady, M. P.; Yamamoto, Y.; Santella, M. L.; Maziasz, P. J.; Pint, B. A.; Liu, C. T.; Lu, Z. P.; Bei, H. (July 2008). "The development of alumina-forming austenitic stainless steels for high-temperature structural use". JOM. 60 (7): 12–18. Bibcode:2008JOM....60g..12B. doi:10.1007/s11837-008-0083-2. S2CID 137354503.
  24. ^ a b c d Muralidharan, G.; Yamamoto, Y.; Brady, M. P.; Walker, L. R.; Meyer III, H. M.; Leonard, D. N. (November 2016). "Development of Cast Alumina-Forming Austenitic Stainless Steels". JOM. 68 (11): 2803–2810. Bibcode:2016JOM....68k2803M. doi:10.1007/s11837-016-2094-8. OSTI 1362187. S2CID 137160315.
  25. ^ Bombač, D.; Fazarinc, M.; Kugler, G.; Spajić, S. (2008). "Microstructure development of Nimonic 80A superalloys during hot deformation". Materials and Geoenvironment. 55 (3): 319–328. Retrieved 8 March 2020 – via ResearchGate.
  26. ^ Reed, R. C (2006). The Superalloys: Fundamentals and Applications. Cambridge: Cambridge University Press. p. 121. ISBN 9780521070119.
  27. ^ Dunand, David C. "High-Temperature Materials for Energy Conversion" Materials Science & Engineering 381: Materials for Energy-Efficient Technology. Northwestern University, Evanston. 3 February 2015. Lecture.
  28. ^ O'Hara, K. S., Walston, W. S., Ross, E. W., Darolia, R. US Patent 5482789, 1996.
  29. ^ Chen, J. Y.; Feng, Q.; Sun, Z. Q. (October 2010). "Topologically close-packed phase promotion in a Ru-containing single crystal superalloy". Scripta Materialia. 63 (8): 795–798. doi:10.1016/j.scriptamat.2010.06.019.
  30. ^ Wahl, Jacqueline; Harris, Ken (2014). "New single crystal superalloys – overview and update" (PDF). MATEC Web of Conferences. 14: 17002. doi:10.1051/matecconf/20141417002.
  31. ^ Nabarro, F. R. N.; de Villiers, H. L. (1995). The Physics of creep : creep and creep-resistant alloys. London: Talylor and Francis. ISBN 9780850668520.
  32. ^ Matan, N.; Cox, D. C.; Carter, P.; Rist, M. A.; Rae, C. M. F.; Reed, R. C. (1999). "Creep of CMSX-4 superalloy single crystals: effects of misorientation and temperature". Acta Materialia. 47 (5): 1549–1563. Bibcode:1999AcMat..47.1549M. doi:10.1016/s1359-6454(99)00029-4.
  33. ^ Nabarro, Frank R. N. (1996). "Rafting in Superalloys". Metallurgical and Materials Transactions A. 27 (3): 513–530. Bibcode:1996MMTA...27..513N. doi:10.1007/BF02648942. S2CID 137172614.
  34. ^ Reed, R. C.; Matan, N.; Cox, D. C.; Rist, M. A.; Rae, C. M. F. (1999). "Creep of CMSX-4 superalloy single crystals: effects of rafting at high temperature". Acta Materialia. 47 (12): 3367–3381. Bibcode:1999AcMat..47.3367R. doi:10.1016/S1359-6454(99)00217-7.
  35. ^ a b Pettit, F.S.; Meier, G.H. (1984). "Oxidation and Hot Corrosion of Superalloys". Superalloys 1984 (Fifth International Symposium). pp. 651–687. doi:10.7449/1984/Superalloys_1984_651_687.
  36. ^ Lund and Wagner. "Oxidation of Nickel- and Cobalt-Base Superalloys"[dead link]. DMIC report 214. 1 March 1965. Defense Metals Information Center, Batelle Memorial Institute, Columbus, Ohio.
  37. ^ Klein, L.; Bauer, S.; Neumeier, S.; Göken, M.; Virtanan, S. (2011). "High temperature oxidation of γ/γ'-strengthened Co-based superalloys". Corrosion Science. 53 (5): 2027–2034. doi:10.1016/j.corsci.2011.02.033.
  38. ^ C. Sims, N. Stoloff, W. Hagel, Superalloys II: High Temperature Materials for Aerospace and Industrial Power, 1987, John Wiley & Sons
  39. ^ "PIM International Vol. 7 No. 1 March 2013". Powder Injection Moulding International. Retrieved 1 March 2016.
  40. ^ Atkinson, H. V.; Davies, S. (December 2000). "Fundamental aspects of hot isostatic pressing: An overview". Metallurgical and Materials Transactions A. 31 (12): 2981–3000. Bibcode:2000MMTA...31.2981A. doi:10.1007/s11661-000-0078-2. S2CID 137660703.
  41. ^ Gu, D D; Meiners, W; Wissenbach, K; Poprawe, R (May 2012). "Laser additive manufacturing of metallic components: materials, processes and mechanisms". International Materials Reviews. 57 (3): 133–164. Bibcode:2012IMRv...57..133G. doi:10.1179/1743280411Y.0000000014. S2CID 137144519.
  42. ^ Graybill, Benjamin; Li, Ming; Malawey, David; Ma, Chao; Alvarado-Orozco, Juan-Manuel; Martinez-Franco, Enrique (18 June 2018). "Additive Manufacturing of Nickel-Based Superalloys". Volume 1: Additive Manufacturing; Bio and Sustainable Manufacturing. College Station, Texas, USA: American Society of Mechanical Engineers. doi:10.1115/MSEC2018-6666. ISBN 978-0-7918-5135-7. S2CID 139639438.
  43. ^ Y. Tamarin, Protective Coatings for Turbine Blades (Materials Park, OH: ASM International, 2002).
  44. ^ J. R. Davis, ed., Handbook of Thermal Spray Technology (Materials Park, OH: The ASM Thermal Spray Society, 2004).
  45. ^ Boone, D. H. (1986). "Physical vapour deposition processes". Materials Science and Technology. 2 (3): 220–224. Bibcode:1986MatST...2..220B. doi:10.1179/mst.1986.2.3.220.
  46. ^ Clarke, David R. (January 2003). "Materials selection guidelines for low thermal conductivity thermal barrier coatings". Surface and Coatings Technology. 163–164: 67–74. CiteSeerX 10.1.1.457.1304. doi:10.1016/S0257-8972(02)00593-5.
  47. ^ "Wadley Research Group '". University of Virginia. Retrieved 3 March 2016.
  48. ^ Warnes, Bruce Michael (January 2003). "Improved aluminide/MCrAlX coating systems for super alloys using CVD low activity aluminizing". Surface and Coatings Technology. 163–164: 106–111. doi:10.1016/S0257-8972(02)00602-3.
  49. ^ Tawancy, H.M.; Abbas, N.M.; Bennett, A. (December 1994). "Role of Y during high temperature oxidation of an M-Cr-Al-Y coating on an Ni-base superalloy". Surface and Coatings Technology. 68–69: 10–16. doi:10.1016/0257-8972(94)90130-9.
  50. ^ D. Chuanxian; H. Bingtang; L. Huiling (24 August 1984). "Plasma-sprayed wear-resistant ceramic and cermet coating materials". Thin Solid Films. 118 (4): 485–493. Bibcode:1984TSF...118..485C. doi:10.1016/0040-6090(84)90277-3.
  51. ^ Kawahara, Yuuzou (January 1997). "Development and application of high-temperature corrosion-resistant materials and coatings for advanced waste-to-energy plants". Materials at High Temperatures. 14 (3): 261–268. Bibcode:1997MaHT...14..261K. doi:10.1080/09603409.1997.11689552.
  52. ^ Longa, Y.; Takemoto, M. (July 1992). "High-Temperature Corrosion of Laser-Glazed Alloys in Na 2 SO 4 -V 2 O 5". Corrosion. 48 (7): 599–607. doi:10.5006/1.3315978.
  53. ^ G. R. Heath, P. Heimgartner, G. Irons, R. Miller, S. Gustafsson, Materials Science Forum 1997, 251–54, 809
  54. ^ Knotek, O. (2001). "Thermal Spraying and Detonation Gun Processes" (PDF). In Bunshah, R. F. (ed.). Handbook of Hard Coatings: Deposition Technologies, Properties and Applications. Park Ridge, NJ: Noyes Pub.; Norwich, NY: William Andrew Pub. pp. 77–107. ISBN 9780815514381.
  55. ^ Niranatlumpong, P.; Ponton, C. B.; Evans, H. E. (2000). "The Failure of Protective Oxides on Plasma-Sprayed NiCrAlY Overlay Coatings". Oxidation of Metals. 53 (3–4): 241–258. doi:10.1023/A:1004549219013. S2CID 136826569.
  56. ^ P. Fauchais, A. Vardelle, M. Vardelle, Modelling of Plasma Spraying of Ceramic Films and Coatings, Ed. Vinenzini, Pub. Elsevier State Publishers B.V 1991.
  57. ^ Evans, A. G.; Mumm, D. R.; Hutchinson, J. W.; Meier, G. H.; Pettit, F. S. (2001). "Mechanisms controlling the durability of thermal barrier coatings". Progress in Materials Science. 46 (5): 505–553. doi:10.1016/s0079-6425(00)00020-7.
  58. ^ Wright, P. K.; Evans, A. G. (1999). "Mechanisms governing the performance of thermal barrier coatings". Current Opinion in Solid State and Materials Science. 4 (3): 255–265. Bibcode:1999COSSM...4..255W. doi:10.1016/s1359-0286(99)00024-8.
  59. ^ Wright, P. K. (1998). "Influence of cyclic strain on life of a PVD TBC". Materials Science and Engineering. A245 (2): 191–200. doi:10.1016/S0921-5093(97)00850-2.
  60. ^ Pint, B.A. (November 2004). "The role of chemical composition on the oxidation performance of aluminide coatings". Surface and Coatings Technology. 188–189: 71–78. doi:10.1016/j.surfcoat.2004.08.007.
  61. ^ Baufeld, B.; Bartsch, M.; Broz, P.; Schmucker, M. (2004). "Microstructural changes as postmortem temperature indicator in Ni-Co-Cr-Al-Y oxidation protection coatings". Materials Science and Engineering. 384 (1–2): 162–171. doi:10.1016/j.msea.2004.05.052.
  62. ^ Nychka, J.A; Clarke, D.R (September 2001). "Damage quantification in TBCs by photo-stimulated luminescence spectroscopy". Surface and Coatings Technology. 146–147: 110–116. doi:10.1016/S0257-8972(01)01455-4.
  63. ^ Mumm, D. R.; Evans, A. G.; Spitsberg, I. T. (2001). "Characterisation of a cyclic displacement instability for a thermally grown oxide in a thermal barrier coating system". Acta Materialia. 49 (12): 2329–2340. doi:10.1016/s1359-6454(01)00071-4.
  64. ^ Mumm, D. R.; Evans, A. G. (2000). "On the role of imperfections in the failure of a thermal barrier coating made by electron beam deposition". Acta Materialia. 48 (8): 1815–1827. Bibcode:2000AcMat..48.1815M. doi:10.1016/s1359-6454(99)00473-5.
  65. ^ Gell, M.; Vaidyanathan, K.; Barber, B.; Cheng, J.; Jordan, E. (1999). "Mechanism of spallation in platinum aluminide/electron beam physical vapor-deposited thermal barrier coatings". Metallurgical and Materials Transactions A. 30 (2): 427–435. Bibcode:1999MMTA...30..427G. doi:10.1007/s11661-999-0332-1. S2CID 137312835.
  66. ^ Evans, A.G.; He, M.Y.; Hutchinson, J.W. (January 2001). "Mechanics-based scaling laws for the durability of thermal barrier coatings". Progress in Materials Science. 46 (3–4): 249–271. doi:10.1016/S0079-6425(00)00007-4.
  67. ^ Schulz, U; Menzebach, M; Leyens, C; Yang, Y.Q (September 2001). "Influence of substrate material on oxidation behavior and cyclic lifetime of EB-PVD TBC systems". Surface and Coatings Technology. 146–147: 117–123. doi:10.1016/S0257-8972(01)01481-5.
  68. ^ Chen, X; Wang, R; Yao, N; Evans, A.G; Hutchinson, J.W; Bruce, R.W (July 2003). "Foreign object damage in a thermal barrier system: mechanisms and simulations". Materials Science and Engineering: A. 352 (1–2): 221–231. doi:10.1016/S0921-5093(02)00905-X.
  69. ^ Walston, W.S. (2004). "Coating and Surface Technologies for Turbine Airfoils". Superalloys 2004 (Tenth International Symposium). pp. 579–588. doi:10.7449/2004/Superalloys_2004_579_588. ISBN 0-87339-576-X.
  70. ^ Mumm, D. R.; Watanabe, M.; Evans, A. G.; Pfaendtner, J. A. (2004). "The influence of test method on failure mechanisms and durability of a thermal barrier system". Acta Materialia. 52 (5): 1123–1131. Bibcode:2004AcMat..52.1123M. CiteSeerX 10.1.1.514.3611. doi:10.1016/j.actamat.2003.10.045.
  71. ^ Brady, M. P.; Muralidharan, G.; Leonard, D. N.; Haynes, J. A.; Weldon, R. G.; England, R. D. (December 2014). "Long-Term Oxidation of Candidate Cast Iron and Stainless Steel Exhaust System Alloys from 650 to 800 °C in Air with Water Vapor". Oxidation of Metals. 82 (5–6): 359–381. doi:10.1007/s11085-014-9496-1. OSTI 1185421. S2CID 136677636.
  72. ^ a b c d Blain, Loz (10 February 2023). "Heat-loving lightweight superalloy promises higher turbine efficiency". New Atlas. Retrieved 12 February 2023.

Bibliography edit

  • Levitin, Valim (2006). High Temperature Strain of Metals and Alloys: Physical Fundamentals. WILEY-VCH. ISBN 978-3-527-31338-9.
  • Shahsavari, H. A.; Kokabi, A. H.; Nategh, S. (2007). "Effect of preweld microstructure on HAZ liquation cracking of Rene 80 superalloy". Materials Science and Technology. 23 (5): 547–555. Bibcode:2007MatST..23..547S. doi:10.1179/174328407x179539. S2CID 135755442.

External links edit

  • "Superalloys". Cambridge University. Extensive bibliography and links.
  • "Nickel-Based Superalloys". Seather. The nickel-based superalloys guides and links.

superalloy, this, article, needs, additional, citations, verification, please, help, improve, this, article, adding, citations, reliable, sources, unsourced, material, challenged, removed, find, sources, news, newspapers, books, scholar, jstor, march, 2018, le. This article needs additional citations for verification Please help improve this article by adding citations to reliable sources Unsourced material may be challenged and removed Find sources Superalloy news newspapers books scholar JSTOR March 2018 Learn how and when to remove this template message A superalloy or high performance alloy is an alloy with the ability to operate at a high fraction of its melting point 1 Key characteristics of a superalloy include mechanical strength thermal creep deformation resistance surface stability and corrosion and oxidation resistance Nickel superalloy jet engine RB199 turbine bladeThe crystal structure is typically face centered cubic FCC austenitic Examples of such alloys are Hastelloy Inconel Waspaloy Rene alloys Incoloy MP98T TMS alloys and CMSX single crystal alloys Superalloy development relies on chemical and process innovations Superalloys develop high temperature strength through solid solution strengthening and precipitation strengthening from secondary phase precipitates such as gamma prime and carbides Oxidation or corrosion resistance is provided by elements such as aluminium and chromium Superalloys are often cast as a single crystal in order to eliminate grain boundaries which decrease creep resistance even though they may provide strength at low temperatures The primary application for such alloys is in aerospace and marine turbine engines Creep is typically the lifetime limiting factor in gas turbine blades 2 Superalloys have made much of very high temperature engineering technology possible 1 Contents 1 Chemical development 1 1 Phase formation 2 Families of superalloys 2 1 Ni based 2 1 1 History 2 1 2 Phases 2 2 Co based 2 2 1 Phases 2 3 Fe based 2 3 1 Microstructure 3 Microstructure 4 Single crystal superalloys 5 Oxidation 6 Processing 6 1 Casting and forging 6 1 1 Investment casting 6 1 2 Directional solidification 6 1 3 Single crystal growth 6 2 Powder metallurgy 6 2 1 Sintering and hot isostatic pressing 6 2 2 Additive manufacturing 7 Coatings 7 1 Types 7 1 1 Thermal barrier coatings 7 1 2 Bond coat 7 2 Process methods 7 2 1 Pack cementation 7 2 2 Thermal spraying 7 2 2 1 Plasma spraying 7 2 3 Gas phase 7 2 4 Failure mechanisms 8 Applications 8 1 Turbines 8 2 Energy production 9 Research 9 1 Radiolysis 9 2 Austentic steel 9 3 AFA superalloys 9 4 Multi principal element superalloy MPES 10 See also 11 References 11 1 Bibliography 12 External linksChemical development editBecause these alloys are intended for high temperature applications their creep and oxidation resistance are of primary importance Nickel Ni based superalloys are the material of choice for these applications because of their unique g precipitates 1 3 page needed The properties of these superalloys can be tailored to a certain extent through the addition of various other elements common or exotic including not only metals but also metalloids and nonmetals chromium iron cobalt molybdenum tungsten tantalum aluminium titanium zirconium niobium rhenium yttrium vanadium carbon boron or hafnium are some examples of the alloying additions used Each addition serves a particular purpose in optimizing properties Creep resistance is dependent in part on slowing the speed of dislocation motion within a crystal structure In modern Ni based superalloys the g Ni3 Al Ti phase acts as a barrier to dislocation For this reason this g intermetallic phase when present in high volume fractions increases the strength of these alloys due to its ordered nature and high coherency with the g matrix The chemical additions of aluminum and titanium promote the creation of the g phase The g phase size can be precisely controlled by careful precipitation strengthening heat treatments Many superalloys are produced using a two phase heat treatment that creates a dispersion of cuboidal g particles known as the primary phase with a fine dispersion between these known as secondary g In order to improve the oxidation resistance of these alloys Al Cr B and Y are added The Al and Cr form oxide layers that passivate the surface and protect the superalloy from further oxidation while B and Y are used to improve the adhesion of this oxide scale to the substrate 4 Cr Fe Co Mo and Re all preferentially partition to the g matrix while Al Ti Nb Ta and V preferentially partition to the g precipitates and solid solution strengthen the matrix and precipitates respectively In addition to solid solution strengthening if grain boundaries are present certain elements are chosen for grain boundary strengthening B and Zr tend to segregate to the grain boundaries which reduces the grain boundary energy and results in better grain boundary cohesion and ductility 5 Another form of grain boundary strengthening is achieved through the addition of C and a carbide former such as Cr Mo W Nb Ta Ti or Hf which drives precipitation of carbides at grain boundaries and thereby reduces grain boundary sliding Ni based superalloy compositions 1 6 7 Element Composition range weight PurposeNi Fe Co 50 70 These elements form the base matrix g phase of the superalloy Ni is necessary because it also forms g Ni3Al Fe and Co have higher melting points than Ni and offer solid solution strengthening Fe is also much cheaper than Ni or Co Cr 5 20 Cr is necessary for oxidation and corrosion resistance it forms a protective oxide Cr2O3 Al 0 5 6 Al is the main g former It also forms a protective oxide Al2O3 which provides oxidation resistance at higher temperature than Cr2O3 Ti 1 4 Ti forms g C 0 05 0 2 MC and M23C6 M metal carbides are the strengthening phase in the absence of g B Zr 0 0 1 Boron and zirconium provide strength to grain boundaries This is not essential in single crystal turbine blades because there are no grain boundaries Nb 0 5 Nb can form g a strengthening phase at lower below 700 C temperatures Re W Hf Mo Ta 1 10 Refractory metals added in small amounts for solid solution strengthening and carbide formation They are heavy but have extremely high melting points Phase formation edit Adding elements is usually helpful because of solid solution strengthening but can result in unwanted precipitation Precipitates can be classified as geometrically close packed GCP topologically close packed TCP or carbides GCP phases usually benefit mechanical properties but TCP phases are often deleterious Because TCP phases are not truly close packed they have few slip systems and are brittle Also they scavenge elements from GCP phases Many elements that are good for forming g or have great solid solution strengthening may precipitate TCPs The proper balance promotes GCPs while avoiding TCPs TCP phase formation areas are weak because they 8 9 have inherently poor mechanical properties are incoherent with the g matrix are surrounded by a depletion zone where there is no g usually form sharp plate or needle like morphologies which nucleate cracksThe main GCP phase is g Almost all superalloys are Ni based because of this phase g is an ordered L12 pronounced L one two which means it has a certain atom on the face of the unit cell and a certain atom on the corners of the unit cell Ni based superalloys usually present Ni on the faces and Ti or Al on the corners Another good GCP phase is g It is also coherent with g but it dissolves at high temperatures Superalloy phases 8 9 Phase Classification Structure Composition s Appearance Effectg matrix disordered FCC Ni Co Fe and other elements in solid solution The background for other precipitates The matrix phase provides ductility and a structure for precipitatesg GCP L12 ordered FCC Ni3 Al Ti cubes rounded cubes spheres or platelets depending on lattice mismatch The main strengthening phase g is coherent with g which allows for ductility Carbide Carbide FCC mC m23C6 and m6C m metal string like clumps like strings of pearls There are many carbides but they all provide dispersion strengthening and grain boundary stabilization g GCP D022 ordered BCT Ni3Nb very small disks This precipitate is coherent with g It is the main strengthening phase in IN 718 but g dissolves at high temperatures h GCP D024 ordered HCP Ni3Ti may form cellular or Widmanstatten patterns The phase is not the worst but it is not as good as g It can be useful in controlling grain boundaries d not close packed orthorhombic Ni3Nb acicular needle like The main issue with this phase is that it s not coherent with g but it is not inherently weak It typically forms from decomposing g but sometimes it s intentionally added in small amounts for grain boundary refinement s TCP tetrahedral FeCr FeCrMo CrCo elongated globules This TCP is usually considered to have the worst mechanical properties 10 It is never desirable for mechanical properties m TCP hexagonal Fe2Nb Co2Ti Fe2Ti globules or platelets This phase has typical TCP issues It is never desirable for mechanical properties Laves TCP rhombohedral Fe Co 7 Mo W 6 coarse Widmanstatten platelets This phase has typical TCP issues It is never desirable for mechanical properties Families of superalloys editNi based edit History edit The United States became interested in gas turbine development around 1905 1 From 1910 1915 austenitic g phase stainless steels were developed to survive high temperatures in gas turbines By 1929 80Ni 20Cr alloy was the norm with small additions of Ti and Al Although early metallurgists did not know it yet they were forming small g precipitates in Ni based superalloys These alloys quickly surpassed Fe and Co based superalloys which were strengthened by carbides and solid solution strengthening Although Cr was great for protecting the alloys from oxidation and corrosion up to 700 C metallurgists began decreasing Cr in favor of Al which had oxidation resistance at much higher temperatures The lack of Cr caused issues with hot corrosion so coatings needed to be developed Around 1950 vacuum melting became commercialized which allowed metallurgists to create higher purity alloys with more precise composition In the 60s and 70s metallurgists changed focus from alloy chemistry to alloy processing Directional solidification was developed to allow columnar or even single crystal turbine blades Oxide dispersion strengthening could obtain very fine grains and superplasticity Phases edit Gamma g This phase composes the matrix of Ni based superalloy It is a solid solution fcc austenitic phase of the alloying elements 10 11 The alloying elements most found in commercial Ni based alloys are C Cr Mo W Nb Fe Ti Al V and Ta During the formation of these materials as they cool from the melt carbides precipitate and at even lower temperatures g phase precipitates 11 12 Gamma prime g This phase constitutes the precipitate used to strengthen the alloy It is an intermetallic phase based on Ni3 Ti Al which have an ordered FCC L12 structure 10 The g phase is coherent with the matrix of the superalloy having a lattice parameter that varies by around 0 5 Ni3 Ti Al are ordered systems with Ni atoms at the cube faces and either Al or Ti atoms at the cube edges As particles of g precipitates aggregate they decrease their energy states by aligning along the lt 100 gt directions forming cuboidal structures 11 This phase has a window of instability between 600 C and 850 C inside of which g will transform into the HCP h phase For applications at temperatures below 650 C the g phase can be utilized for strengthening 13 nbsp Crystal structure for g Ni3Nb Body Centered Tetragonal Gamma double prime g This phase typically is Ni3Nb or Ni3V and is used to strengthen Ni based superalloys at lower temperatures lt 650 C relative to g The crystal structure of g is body centered tetragonal BCT and the phase precipitates as 60 nm by 10 nm discs with the 001 planes in g parallel to the 001 family in g These anisotropic discs form as a result of lattice mismatch between the BCT precipitate and the FCC matrix This lattice mismatch leads to high coherency strains which together with order hardening are the primary strengthening mechanisms The g phase is unstable above approximately 650 C 13 Carbide phases Carbide formation is usually deleterious although in Ni based superalloys they are used to stabilize the structure of the material against deformation at high temperatures Carbides form at the grain boundaries inhibiting grain boundary motion 10 11 Topologically close packed TCP phases The term TCP phase refers to any member of a family of phases including the s phase the x phase the m phase and the Laves phase which are not atomically close packed but possess some close packed planes with HCP stacking TCP phases tend to be highly brittle and deplete the g matrix of strengthening solid solution refractory elements including Cr Co W and Mo These phases form as a result of kinetics after long periods of time thousands of hours at high temperatures gt 750 C 13 Co based edit Co based superalloys depend on carbide precipitation and solid solution strengthening for mechanical properties While these strengthening mechanisms are inferior to gamma prime g precipitation strengthening 1 cobalt has a higher melting point than nickel and has superior hot corrosion resistance and thermal fatigue As a result carbide strengthened Co based superalloys are used in lower stress higher temperature applications such as stationary vanes in gas turbines 14 Co s g g microstructure was rediscovered and published in 2006 by Sato et al 15 That g phase was Co3 Al W Mo Ti Nb V and Ta partition to the g phase while Fe Mn and Cr partition to the matrix g The next family of Co based superalloys was discovered in 2015 by Makineni et al This family has a similar g g microstructure but is W free and has a g phase of Co3 Al Mo Nb 16 Since W is heavy its elimination makes Co based alloys increasingly viable in turbines for aircraft where low density is especially valued The most recently discovered family of superalloys was computationally predicted by Nyshadham et al in 2017 17 and demonstrated by Reyes Tirado et al in 2018 18 This g phase is W free and has the composition Co3 Nb V and Co3 Ta V Phases edit Gamma g This is the matrix phase While Co based superalloys are less used commercially alloying elements include C Cr W Ni Ti Al Ir and Ta 15 19 As in stainless steels Chromium is used occasionally up to 20 wt to improve resistance to oxidation and corrosion via the formation of a Cr2O3 passive layer which is critical for use in gas turbines but also provides solid solution strengthening due to the mismatch in the atomic radii of Co and Cr and precipitation hardening due to the formation of MC type carbides 20 Gamma Prime g Constitutes the precipitate used to strengthen the alloy It is usually close packed with a L12 structure of Co3Ti or FCC Co3Ta though both W and Al integrate into these cuboidal precipitates Ta Nb and Ti integrate into the g phase and are stabilize it at high temperatures 15 21 Carbide Phases Carbides strengthen the alloy through precipitation hardening but decrease low temperature ductility 19 Topologically Close Packed TCP phases may appear in some Co based superalloys but embrittle the alloy and are thus undesirable Fe based edit Steel superalloys are of interest because some present creep and oxidation resistance similar to Ni based superalloys at far less cost Gamma g Fe based alloys feature a matrix phase of austenite iron FCC Alloying elements include Al B C Co Cr Mo Ni Nb Si Ti W and Y 22 Al oxidation benefits must be kept at low weight fractions wt because Al stabilizes a ferritic BCC primary phase matrix which is undesirable as it is inferior to the high temperature strength exhibited by an austenitic FCC primary phase matrix 23 Gamma prime g This phase is introduced as precipitates to strengthen the alloy g Ni3Al precipitates can be introduced with the proper balance of Al Ni Nb and Ti additions Microstructure edit The two major types of austenitic stainless steels are characterized by the oxide layer that forms on the steel surface either chromia forming or alumina forming Cr forming stainless steel is the most common type However Cr forming steels do not exhibit high creep resistance at high temperatures especially in environments with water vapor Exposure to water vapor at high temperatures can increase internal oxidation in Cr forming alloys and rapid formation of volatile Cr oxy hydroxides both of which can reduce durability and lifetime 23 Al forming austenitic stainless steels feature a single phase matrix of austenite iron FCC with an Al oxide at the surface of the steel Al is more thermodynamically stable in oxygen than Cr More commonly however precipitate phases are introduced to increase strength and creep resistance In Al forming steels NiAl precipitates are introduced to act as Al reservoirs to maintain the protective alumina layer In addition Nb and Cr additions help form and stabilize Al by increasing precipitate volume fractions of NiAl 23 At least 5 grades of alumina forming austenitic AFA alloys with different operating temperatures at oxidation in air 10 water vapor have been realized 24 AFA Grade 50 60 Fe 20 25 Ni 14 15 Cr 2 5 3 5 Al 1 3 Nb wt base 750 800 C operating temperatures at oxidation in air 10 water vapor Low Nickel AFA Grade 63Fe 12Ni 14Cr 2 5Al 0 6Nb 5Mn3Cu wt base 650 C operating temperatures at oxidation in air 10 water vapor High Performance AFA Grade 45 55 Fe 25 30 Ni 14 15 Cr 3 5 4 5 Al 1 3 Nb 0 02 0 1 Hf Y wt base 850 900 C operating temperatures at oxidation in air 10 water vapor Cast AFA Grade 35 50 Fe 25 35 Ni 14Cr 3 5 4 Al 1Nb wt base 750 1100 C operating temperatures at oxidation in air 10 water vapor depending upon Ni wt AFA superalloy 40 50 Fe 30 35 Ni 14 19 Cr 2 5 3 5 Al 3Nb 750 850 C operating temperatures at oxidation in air 10 water vaporOperating temperatures with oxidation in air and no water vapor are expected to be higher In addition an AFA superalloy grade exhibits creep strength approaching that of nickel alloy UNS N06617 Microstructure editIn pure Ni3Al phase Al atoms are placed at the vertices of the cubic cell and form sublattice A Ni atoms are located at centers of the faces and form sublattice B The phase is not strictly stoichiometric An excess of vacancies in one of the sublattices may exist which leads to deviations from stoichiometry Sublattices A and B of the g phase can solute a considerable proportion of other elements The alloying elements are dissolved in the g phase The g phase hardens the alloy through the yield strength anomaly Dislocations dissociate in the g phase leading to the formation of an anti phase boundary At elevated temperature the free energy associated with the anti phase boundary APB is considerably reduced if it lies on a particular plane which by coincidence is not a permitted slip plane One set of partial dislocations bounding the APB cross slips so that the APB lies on the low energy plane and since this low energy plane is not a permitted slip plane the dissociated dislocation is effectively locked By this mechanism the yield strength of g phase Ni3Al increases with temperature up to about 1000 C Initial material selection for blade applications in gas turbine engines included alloys like the Nimonic series alloys in the 1940s 3 page needed The early Nimonic series incorporated g Ni3 Al Ti precipitates in a g matrix as well as various metal carbon carbides e g Cr23C6 at the grain boundaries 25 for additional grain boundary strength Turbine blade components were forged until vacuum induction casting technologies were introduced in the 1950s 3 page needed This process significantly improved cleanliness reduced defects and increased the strength and temperature capability Modern superalloys were developed in the 1980s First generation superalloys incorporated increased Al Ti Ta and Nb content in order to increase the g volume fraction Examples include PWA1480 Rene N4 and SRR99 Additionally the volume fraction of the g precipitates increased to about 50 70 with the advent of monocrystal solidification techniques that enable grain boundaries to be entirely eliminated Because the material contains no grain boundaries carbides are unnecessary as grain boundary strengthers and were thus eliminated 3 page needed Second and third generation superalloys introduce about 3 and 6 weight percent rhenium for increased temperature capability Re is a slow diffuser and typically partitions the g matrix decreasing the rate of diffusion and thereby high temperature creep and improving high temperature performance and increasing service temperatures by 30 C and 60 C in second and third generation superalloys respectively 26 Re promotes the formation of rafts of the g phase as opposed to cuboidal precipitates The presence of rafts can decrease creep rate in the power law regime controlled by dislocation climb but can also potentially increase the creep rate if the dominant mechanism is particle shearing Re tends to promote the formation of brittle TCP phases which has led to the strategy of reducing Co W Mo and particularly Cr Later generations of Ni based superalloys significantly reduced Cr content for this reason however with the reduction in Cr comes a reduction in oxidation resistance Advanced coating techniques offset the loss of oxidation resistance accompanying the decreased Cr contents 13 27 Examples of second generation superalloys include PWA1484 CMSX 4 and Rene N5 Third generation alloys include CMSX 10 and Rene N6 Fourth fifth and sixth generation superalloys incorporate ruthenium additions making them more expensive than prior Re containing alloys The effect of Ru on the promotion of TCP phases is not well determined Early reports claimed that Ru decreased the supersaturation of Re in the matrix and thereby diminished the susceptibility to TCP phase formation 28 Later studies noted an opposite effect Chen et al found that in two alloys differing significantly only in Ru content USTB F3 and USTB F6 that the addition of Ru increased both the partitioning ratio as well as supersaturation in the g matrix of Cr and Re and thereby promoted the formation of TCP phases 29 The current trend is to avoid very expensive and very heavy elements An example is Eglin steel a budget material with compromised temperature range and chemical resistance It does not contain rhenium or ruthenium and its nickel content is limited To reduce fabrication costs it was chemically designed to melt in a ladle though with improved properties in a vacuum crucible Conventional welding and casting is possible before heat treatment The original purpose was to produce high performance inexpensive bomb casings but the material has proven widely applicable to structural applications including armor Single crystal superalloys editSingle crystal superalloys SX or SC superalloys are formed as a single crystal using a modified version of the directional solidification technique leaving no grain boundaries The mechanical properties of most other alloys depend on the presence of grain boundaries but at high temperatures they participate in creep and require other mechanisms In many such alloys islands of an ordered intermetallic phase sit in a matrix of disordered phase all with the same crystal lattice This approximates the dislocation pinning behavior of grain boundaries without introducing any amorphous solid into the structure Single crystal SX superalloys have wide application in the high pressure turbine section of aero and industrial gas turbine engines due to the unique combination of properties and performance Since introduction of single crystal casting technology SX alloy development has focused on increased temperature capability and major improvements in alloy performance are associated with rhenium Re and ruthenium Ru 30 The creep deformation behavior of superalloy single crystal is strongly temperature stress orientation and alloy dependent For a single crystal superalloy three modes of creep deformation occur under regimes of different temperature and stress rafting tertiary and primary 31 page needed At low temperature 750 C SX alloys exhibits mostly primary creep behavior Matan et al concluded that the extent of primary creep deformation depends strongly on the angle between the tensile axis and the lt 001 gt lt 011 gt symmetry boundary 32 At temperatures above 850 C tertiary creep dominates and promotes strain softening behavior 3 page needed When temperature exceeds 1000 C the rafting effect is prevalent where cubic particles transform into flat shapes under tensile stress 33 The rafts form perpendicular to the tensile axis since g phase is transported out of the vertical channels and into the horizontal ones Reed et al studied unaxial creep deformation of lt 001 gt oriented CMSX 4 single crystal superalloy at 1105 C and 100 MPa They reported that rafting is beneficial to creep life since it delays evolution of creep strain In addition rafting occurs quickly and suppresses the accumulation of creep strain until a critical strain is reached 34 Oxidation editFor superalloys operating at high temperatures and exposed to corrosive environments oxidation behavior is a concern Oxidation involves chemical reactions of the alloying elements with oxygen to form new oxide phases generally at the alloy surface If unmitigated oxidation can degrade the alloy over time in a variety of ways including 35 36 sequential surface oxidation cracking and spalling eroding the alloy over time surface embrittlement through the introduction of oxide phases promoting crack formation and fatigue failure depletion of key alloying elements affecting mechanical properties and possibly compromising performanceSelective oxidation is the primary strategy used to limit these deleterious processes The ratio of alloying elements promotes formation of a specific oxide phase that then acts as a barrier to further oxidation Most commonly aluminum and chromium are used in this role because they form relatively thin and continuous oxide layers of alumina Al2O3 and chromia Cr2O3 respectively They offer low oxygen diffusivities effectively halting further oxidation beneath this layer In the ideal case oxidation proceeds through two stages First transient oxidation involves the conversion of various elements especially the majority elements e g nickel or cobalt Transient oxidation proceeds until the selective oxidation of the sacrificial element forms a complete barrier layer 35 The protective effect of selective oxidation can be undermined The continuity of the oxide layer can be compromised by mechanical disruption due to stress or may be disrupted as a result of oxidation kinetics e g if oxygen diffuses too quickly If the layer is not continuous its effectiveness as a diffusion barrier to oxygen is compromised The stability of the oxide layer is strongly influenced by the presence of other minority elements For example the addition of boron silicon and yttrium to superalloys promotes oxide layer adhesion reducing spalling and maintaining continuity 37 Oxidation is the most basic form of chemical degradation superalloys may experience More complex corrosion processes are common when operating environments include salts and sulfur compounds or under chemical conditions that change dramatically over time These issues are also often addressed through comparable coatings Processing editSuperalloys were originally iron based and cold wrought prior to the 1940s when investment casting of cobalt base alloys significantly raised operating temperatures The 1950s development of vacuum melting allowed for fine control of the chemical composition of superalloys and reduction in contamination and in turn led to a revolution in processing techniques such as directional solidification of alloys and single crystal superalloys 38 page needed Processing methods vary widely depending on the required properties of each item Casting and forging edit Casting and forging are traditional metallurgical processing techniques that can be used to generate both polycrystalline and monocrystalline products Polycrystalline casts offer higher fracture resistance while monocrystalline casts offer higher creep resistance Jet turbine engines employ both crystalline component types to take advantage of their individual strengths The disks of the high pressure turbine which are near the central hub of the engine are polycrystalline The turbine blades which extend radially into the engine housing experience a much greater centripetal force necessitating creep resistance typically adopting monocrystalline or polycrystalline with a preferred crystal orientation Investment casting edit Investment casting is a metallurgical processing technique in which a wax form is fabricated and used as a template for a ceramic mold A ceramic mold is poured around the wax form and solidifies the wax form is melted out of the ceramic mold and molten metal is poured into the void left by the wax This leads to a metal form in the same shape as the original wax form Investment casting leads to a polycrystalline final product as nucleation and growth of crystal grains occurs at numerous locations throughout the solid matrix Generally the polycrystalline product has no preferred grain orientation Directional solidification edit nbsp Schematic of directional solidificationDirectional solidification uses a thermal gradient to promote nucleation of metal grains on a low temperature surface as well as to promote their growth along the temperature gradient This leads to grains elongated along the temperature gradient and significantly greater creep resistance parallel to the long grain direction In polycrystalline turbine blades directional solidification is used to orient the grains parallel to the centripetal force It is also known as dendritic solidification Single crystal growth edit Single crystal growth starts with a seed crystal that is used to template growth of a larger crystal The overall process is lengthy and machining is necessary after the single crystal is grown Powder metallurgy edit Powder metallurgy is a class of modern processing techniques in which metals are first powdered and then formed into the desired shape by heating below the melting point This is in contrast to casting which occurs with molten metal Superalloy manufacturing often employs powder metallurgy because of its material efficiency typically much less waste metal must be machined away from the final product and its ability to facilitate mechanical alloying Mechanical alloying is a process by which reinforcing particles are incorporated into the superalloy matrix material by repeated fracture and welding 39 failed verification Sintering and hot isostatic pressing edit Sintering and hot isostatic pressing are processing techniques used to densify materials from a loosely packed green body into a solid object with physically merged grains Sintering occurs below the melting point and causes adjacent particles to merge at their boundaries creating a strong bond between them In hot isostatic pressing a sintered material is placed in a pressure vessel and compressed from all directions isostatically in an inert atmosphere to affect densification 40 Additive manufacturing edit Selective laser melting also known as powder bed fusion is an additive manufacturing procedure used to create intricately detailed forms from a CAD file A shape is designed and then converted into slices These slices are sent to a laser writer to print the final product In brief a bed of metal powder is prepared and a slice is formed in the powder bed by a high energy laser sintering the particles together The powder bed moves downwards and a new batch of metal powder is rolled over the top This layer is then sintered with the laser and the process is repeated until all slices have been processed 41 Additive manufacturing can leave pores behind Many products undergo a heat treatment or hot isostatic pressing procedure to densify the product and reduce porosity 42 Coatings editIn modern gas turbines the turbine entry temperature 1750K exceeds superalloy incipient melting temperature 1600K with the help of surface engineering 43 page needed Types edit The three types of coatings are diffusion coatings overlay coatings and thermal barrier coatings Diffusion coatings mainly constituted with aluminide or platinum aluminide is the most common MCrAlX based overlay coatings M Ni or Co X Y Hf Si enhance resistance to corrosion and oxidation Compared to diffusion coatings overlay coatings are more expensive but less dependent on substrate composition since they must be carried out by air or vacuum plasma spraying APS VPS 44 page needed or electron beam physical vapour deposition EB PVD 45 Thermal barrier coatings provide by far the best enhancement in working temperature and coating life It is estimated that modern TBC of thickness 300 mm if used in conjunction with a hollow component and cooling air has the potential to lower metal surface temperatures by a few hundred degrees 46 Thermal barrier coatings edit Thermal barrier coatings TBCs are used extensively in gas turbine engines to increase component life and engine performance 47 A coating of about 1 200 µm can reduce the temperature at the superalloy surface by up to 200 K TBCs are a system of coatings consisting of a bond coat a thermally grown oxide TGO and a thermally insulating ceramic top coat In most applications the bond coat is either a MCrAlY where M Ni or NiCo or a Pt modified aluminide coating A dense bond coat is required to provide protection of the superalloy substrate from oxidation and hot corrosion attack and to form an adherent slow growing surface TGO The TGO is formed by oxidation of the aluminum that is contained in the bond coat The current first generation thermal insulation layer is composed of 7wt yttria stabilized zirconia 7YSZ with a typical thickness of 100 300 µm Yttria stabilized zirconia is used due to its low thermal conductivity 2 6W mK for fully dense material relatively high coefficient of thermal expansion and high temperature stability The electron beam directed vapor deposition EB DVD process used to apply the TBC to turbine airfoils produces a columnar microstructure with multiple porosity levels Inter column porosity is critical to providing strain tolerance via a low in plane modulus as it would otherwise spall on thermal cycling due to thermal expansion mismatch with the superalloy substrate This porosity reduces the thermal coating s conductivity Bond coat edit The bond coat adheres the thermal barrier to the substrate Additionally the bond coat provides oxidation protection and functions as a diffusion barrier against the motion of substrate atoms towards the environment The five major types of bond coats are the aluminides the platinum aluminides MCrAlY cobalt cermets and nickel chromium For aluminide bond coatings the coating s final composition and structure depends on the substrate composition Aluminides lack ductility below 750 C and exhibit limited thermomechanical fatigue strength Pt aluminides are similar to the aluminide bond coats except for a layer of Pt 5 10 mm deposited on the blade The Pt aids in oxide adhesion and contributes to hot corrosion increasing blade lifespan MCrAlY does not strongly interact with the substrate Normally applied by plasma spraying MCrAlY coatings from secondary aluminum oxides This means that the coatings form an outer chromia layer and a secondary alumina layer underneath These oxide formations occur at high temperatures in the range of those that superalloys usually encounter 48 The chromia provides oxidation and hot corrosion resistance The alumina controls oxidation mechanisms by limiting oxide growth by self passivating The yttrium enhances oxide adherence to the substrate and limits the growth of grain boundaries which can lead to coat flaking 49 Addition of rhenium and tantalum increases oxidation resistance Cobalt cermet based coatings consisting of materials such as tungsten carbide cobalt can be used due to excellent resistance to abrasion corrosion erosion and heat 50 full citation needed These cermet coatings perform well in situations where temperature and oxidation damage are significant concerns such as boilers One of cobalt cermet s unique advantages is minimal loss of coating mass over time due to the strength of carbides Overall cermet coatings are useful in situations where mechanical demands are equal to chemical demands Nickel chromium coatings are used most frequently in boilers fed by fossil fuels electric furnaces and waste incineration furnaces where the danger of oxidizing agents and corrosive compounds in the vapor must be addressed 51 The specific method of spray coating depends on the coating composition Nickel chromium coatings that also contain iron or aluminum provide better corrosion resistance when they are sprayed and laser glazed while pure nickel chromium coatings perform better when thermally sprayed exclusively 52 Process methods edit Several kinds of coating process are available pack cementation process gas phase coating both are a type of chemical vapor deposition CVD thermal spraying and physical vapor deposition In most cases after the coating process near surface regions of parts are enriched with aluminium in a matrix of the nickel aluminide Pack cementation edit Pack cementation is a widely used CVD technique that consists of immersing the components to be coated in a metal powder mixture and ammonium halide activators and sealing them in a retort The entire apparatus is placed inside a furnace and heated in a protective atmosphere to a lower than normal temperature that allows diffusion due to the halide salts chemical reaction that causes a eutectic bond between the two metals The surface alloy that is formed due to thermal diffused ion migration has a metallurgical bond to the substrate and an intermetallic layer found in the gamma layer of the surface alloys The traditional pack consists of four components at temperatures below 750 C Substrate or partsFerrous and non ferrous powdered alloy Ti and or Al Si and or Zn B and or Cr Halide salt activator Ammonium halide saltsRelatively inert filler powder Al2O3 SiO2 or SiC This process includes Aluminizing Chromizing Siliconizing Sherardizing Boronizing TitaniumizingPack cementation has reemerged when combined with other chemical processes to lower the temperatures of metal combinations and give intermetallic properties to different alloy combinations for surface treatments Thermal spraying edit Thermal spraying involves heating a feedstock of precursor material and spraying it on a surface Specific techniques depend on desired particle size coat thickness spray speed desired area etc 53 full citation needed Thermal spraying relies on adhesion to the surface As a result the surface of the superalloy must be cleaned and prepared and usually polished before application 54 Plasma spraying edit Plasma spraying offers versatility of usable coatings and high temperature performance 55 Plasma spraying can accommodate a wide range of materials versus other techniques As long as the difference between melting and decomposition temperatures is greater than 300 K plasma spraying is viable 56 page needed Gas phase edit Gas phase coating is carried out at higher temperatures about 1080 C The coating material is usually loaded onto trays without physical contact with the parts to be coated The coating mixture contains active coating material and activator but usually not thermal ballast As in the pack cementation process gaseous aluminium chloride or fluoride is transferred to the surface of the part However in this case the diffusion is outwards This kind of coating also requires diffusion heat treatment Failure mechanisms edit Failure of thermal barrier coating usually manifests as delamination which arises from the temperature gradient during thermal cycling between ambient temperature and working conditions coupled with the difference in thermal expansion coefficient of substrate and coating It is rare for the coating to fail completely some pieces remain intact and significant scatter is observed in the time to failure if testing is repeated under identical conditions 3 page needed Various degradation mechanisms affect thermal barrier coating 57 58 and some or all of these must operate before failure finally occurs Oxidation at the interface of thermal barrier coating and underlying bond coat 59 Depletion of aluminum in bond coat due to oxidation 60 and diffusion with substrate 61 Thermal stresses from mismatch in thermal expansion coefficient and growth stress due to the formation of thermally grown oxide layer 62 Imperfections near thermally grown oxide layer 63 64 65 Various other complicating factors during engine operation 66 67 68 69 70 Additionally TBC life is sensitive to the combination of materials substrate bond coat ceramic and processes EB PVD plasma spraying used Applications editThis section needs additional citations for verification Please help improve this article by adding citations to reliable sources in this section Unsourced material may be challenged and removed April 2022 Learn how and when to remove this template message Turbines edit Nickel based superalloys are used in load bearing structures requiring the highest homologous temperature of any common alloy system Tm 0 9 or 90 of their melting point Among the most demanding applications for a structural material are those in the hot sections of turbine engines e g turbine blade They comprise over 50 of the weight of advanced aircraft engines The widespread use of superalloys in turbine engines coupled with the fact that the thermodynamic efficiency of turbine engines is a function of increasing turbine inlet temperatures has provided part of the motivation for increasing the maximum use temperature of superalloys From 1990 2020 turbine airfoil temperature capability increased on average by about 2 2 C year Two major factors have made this increase possible citation needed Processing techniques that improved alloy cleanliness thus improving reliability and or enabled the production of tailored microstructures such as directionally solidified or single crystal material Alloy development resulting in higher temperature materials primarily through the additions of refractory elements such as Re W Ta and Mo About 60 of the temperature increases related to advanced cooling while 40 have resulted from material improvements State of the art turbine blade surface temperatures approach 1 150 C The most severe stress and temperature combinations correspond to an average bulk metal temperature approaching 1 000 C Although Ni based superalloys retain significant strength to 980 C they tend to be susceptible to environmental attack because of the presence of reactive alloying elements Surface attack includes oxidation hot corrosion and thermal fatigue 10 Energy production edit High temperature materials are valuable for energy conversion and energy production applications Maximum energy conversion efficiency is desired in such applications in accord with the Carnot cycle Because Carnot efficiency is limited by the temperature difference between the hot and cold reservoirs higher operating temperatures increase energy conversion efficiency Operating temperatures are limited by superalloys limiting applications to around 1000 C 1400 C Energy applications include 71 Solar thermal power plants stainless steel rods containing heated water Steam turbines turbine blades and boiler housing Heat exchangers for nuclear reactor systemsAlumina forming stainless steel is weldable and has potential for use in automotive applications such as for high temperature exhaust piping and in heat capture and reuse Research editThis section needs additional citations for verification Please help improve this article by adding citations to reliable sources in this section Unsourced material may be challenged and removed April 2022 Learn how and when to remove this template message Radiolysis edit Sandia National Laboratories is studying radiolysis for making superalloys It uses nanoparticle synthesis to create alloys and superalloys This process holds promise as a universal method of nanoparticle formation By developing an understanding of the basic material science it might be possible to expand research into other aspects of superalloys Radiolysis produces polycrystalline alloys which suffer from an unacceptable level of creep Austentic steel edit Stainless steel alloys remain a research target because of lower production costs as well as the need for an austenitic stainless steel with high temperature corrosion resistance in environments with water vapor Research focuses on increasing high temperature tensile strength toughness and creep resistance to compete with Ni based superalloys 24 Oak Ridge National Laboratory is researching austentic alloys achieving similar creep and corrosion resistance at 800 C to that of other austenitic alloys including Ni based superalloys 24 AFA superalloys edit Development of AFA superalloys with a 35 wt Ni base have shown potential for use in operating temperatures upwards to 1 100 C 24 Multi principal element superalloy MPES edit Researchers at Sandia Labs Ames National Laboratory and Iowa State University reported a 3D printed superalloy composed of 42 aluminum 25 titanium 13 niobium 8 zirconium 8 molybdenum and 4 tantalum Most alloys are made chiefly of one primary element combined with low amounts of other elements In contrast MPES have substantial amounts of three or more elements 72 Such alloys promise improvements on high temperature applications strength to weight fracture toughness corrosion and radiation resistance wear resistance and others They reported hardness and density of 1 8 2 6 GPa cm3 g which surpasses all known alloys including intermetallic compounds titanium aluminides refractory MPEAs and conventional Ni based superalloys This represents a 300 improvement over Inconel 718 based on measured peak hardness of 4 5 GPa and density of 8 2 g cm3 0 55 GPa cm3 g 72 The material is stable at 800 C hotter than the 570 C found in typical coal based power plants 72 The researchers acknowedged that the 3D printing process produces microscopic cracks when forming large parts and that the feedstock includes metals that limit applicability in cost sensitive applications 72 See also editOxide dispersion strengthened alloy Titanium aluminideReferences edit a b c d e f Sims C T 1984 A History of Superalloy Metallurgy for Superalloy Metallurgists Superalloys 1984 Fifth International Symposium pp 399 419 doi 10 7449 1984 Superalloys 1984 399 419 Carter Tim J April 2005 Common failures in gas turbine blades Engineering Failure Analysis 12 2 237 247 doi 10 1016 j engfailanal 2004 07 004 a b c d e f Reed R C 2008 The Superalloys Fundamentals and Applications Cambridge Cambridge University Press ISBN 9780521070119 Klein L Shen Y Killian M S Virtanen S 2011 Effect of B and Cr on the high temperature oxidation behaviour of novel g g strengthened Co base superalloys Corrosion Science 53 9 2713 720 doi 10 1016 j corsci 2011 04 020 Shinagawa K Omori Toshihiro Oikawa Katsunari Kainuma Ryosuke Ishida Kiyohito 2009 Ductility Enhancement by Boron Addition in Co Al W High temperature Alloys Scripta Materialia 61 6 612 15 doi 10 1016 j scriptamat 2009 05 037 Giamei Anthony September 2013 Development of Single Crystal Superalloys A Brief History Advanced Materials amp Processes 26 30 via asminternational Akca Enes Gursel Ali 2015 A Review on Superalloys and IN718 Nickel Based INCONEL Superalloy Periodicals of Engineering and Natural Sciences 3 1 15 27 doi 10 21533 pen v3i1 43 via pen ius edu ba a b Belan Juraj 2016 GCP and TCP Phases Presented in Nickel base Superalloys Materials Today Proceedings 3 4 936 941 doi 10 1016 j matpr 2016 03 024 a b Rae C M F Karunaratne M S A Small C J Broomfield R W Jones C N Reed R C 2000 Topologically Close Packed Phases in an Experimental Rhenium Containing Single Crystal Superalloy Superalloys 2000 Ninth International Symposium pp 767 776 doi 10 7449 2000 Superalloys 2000 767 776 ISBN 0 87339 477 1 a b c d e Randy Bowman Superalloys A Primer and History Retrieved 6 March 2020 via tms org a b c d Sabol G P Stickler R 1969 Microstructure of Nickel Based Superalloys Physica Status Solidi B 35 1 11 52 Bibcode 1969PSSBR 35 11S doi 10 1002 pssb 19690350102 Doi M Miki D Moritani T Kozakai T 2004 Gamma Gamma Prime Microstructure Formed by Phased Separation of Gamma Prime Precipitates in a Ni Al Ti Alloy Superalloys 2004 Tenth International Symposium pp 109 114 doi 10 7449 2004 Superalloys 2004 109 114 ISBN 0 87339 576 X a b c d Dunand David C Materials Science amp Engineering 435 High Temperature Materials Northwestern University Evanston 25 February 2016 Lecture Institute Cobalt 14 February 2018 Superalloys www cobaltinstitute org Retrieved 10 December 2019 a b c Sato J 2006 Cobalt Base High Temperature Alloys Science 312 5770 90 91 Bibcode 2006Sci 312 90S doi 10 1126 science 1121738 PMID 16601187 S2CID 23877638 Makineni S K Nithin B Chattopadhyay K March 2015 A new tungsten free g g Co Al Mo Nb based superalloy Scripta Materialia 98 36 39 doi 10 1016 j scriptamat 2014 11 009 Nyshadham Chandramouli Oses Corey Hansen Jacob E Takeuchi Ichiro Curtarolo Stefano Hart Gus L W January 2017 A computational high throughput search for new ternary superalloys Acta Materialia 122 438 447 arXiv 1603 05967 Bibcode 2017AcMat 122 438N doi 10 1016 j actamat 2016 09 017 S2CID 11222811 Reyes Tirado Fernando L Perrin Toinin Jacques Dunand David C June 2018 g g microstructures in the Co Ta V and Co Nb V ternary systems Acta Materialia 151 137 148 doi 10 1016 j actamat 2018 03 057 a b Cui C 2006 A New Co Base Superalloy Strengthened by g Phase Materials Transactions 47 8 2099 2102 doi 10 2320 matertrans 47 2099 Coutsouradis D Davin A Lamberigts M April 1987 Cobalt based superalloys for applications in gas turbines Materials Science and Engineering 88 11 19 doi 10 1016 0025 5416 87 90061 9 Suzuki A Pollock Tresa M 2008 High temperature strength and deformation of g g two phase Co Al W base alloys Acta Materialia 56 6 1288 97 doi 10 1016 j actamat 2007 11 014 Review precipitation in austenitic stainless steels www phase trans msm cam ac uk Retrieved 2 March 2018 a b c Brady M P Yamamoto Y Santella M L Maziasz P J Pint B A Liu C T Lu Z P Bei H July 2008 The development of alumina forming austenitic stainless steels for high temperature structural use JOM 60 7 12 18 Bibcode 2008JOM 60g 12B doi 10 1007 s11837 008 0083 2 S2CID 137354503 a b c d Muralidharan G Yamamoto Y Brady M P Walker L R Meyer III H M Leonard D N November 2016 Development of Cast Alumina Forming Austenitic Stainless Steels JOM 68 11 2803 2810 Bibcode 2016JOM 68k2803M doi 10 1007 s11837 016 2094 8 OSTI 1362187 S2CID 137160315 Bombac D Fazarinc M Kugler G Spajic S 2008 Microstructure development of Nimonic 80A superalloys during hot deformation Materials and Geoenvironment 55 3 319 328 Retrieved 8 March 2020 via ResearchGate Reed R C 2006 The Superalloys Fundamentals and Applications Cambridge Cambridge University Press p 121 ISBN 9780521070119 Dunand David C High Temperature Materials for Energy Conversion Materials Science amp Engineering 381 Materials for Energy Efficient Technology Northwestern University Evanston 3 February 2015 Lecture O Hara K S Walston W S Ross E W Darolia R US Patent 5482789 1996 Chen J Y Feng Q Sun Z Q October 2010 Topologically close packed phase promotion in a Ru containing single crystal superalloy Scripta Materialia 63 8 795 798 doi 10 1016 j scriptamat 2010 06 019 Wahl Jacqueline Harris Ken 2014 New single crystal superalloys overview and update PDF MATEC Web of Conferences 14 17002 doi 10 1051 matecconf 20141417002 Nabarro F R N de Villiers H L 1995 The Physics of creep creep and creep resistant alloys London Talylor and Francis ISBN 9780850668520 Matan N Cox D C Carter P Rist M A Rae C M F Reed R C 1999 Creep of CMSX 4 superalloy single crystals effects of misorientation and temperature Acta Materialia 47 5 1549 1563 Bibcode 1999AcMat 47 1549M doi 10 1016 s1359 6454 99 00029 4 Nabarro Frank R N 1996 Rafting in Superalloys Metallurgical and Materials Transactions A 27 3 513 530 Bibcode 1996MMTA 27 513N doi 10 1007 BF02648942 S2CID 137172614 Reed R C Matan N Cox D C Rist M A Rae C M F 1999 Creep of CMSX 4 superalloy single crystals effects of rafting at high temperature Acta Materialia 47 12 3367 3381 Bibcode 1999AcMat 47 3367R doi 10 1016 S1359 6454 99 00217 7 a b Pettit F S Meier G H 1984 Oxidation and Hot Corrosion of Superalloys Superalloys 1984 Fifth International Symposium pp 651 687 doi 10 7449 1984 Superalloys 1984 651 687 Lund and Wagner Oxidation of Nickel and Cobalt Base Superalloys dead link DMIC report 214 1 March 1965 Defense Metals Information Center Batelle Memorial Institute Columbus Ohio Klein L Bauer S Neumeier S Goken M Virtanan S 2011 High temperature oxidation of g g strengthened Co based superalloys Corrosion Science 53 5 2027 2034 doi 10 1016 j corsci 2011 02 033 C Sims N Stoloff W Hagel Superalloys II High Temperature Materials for Aerospace and Industrial Power 1987 John Wiley amp Sons PIM International Vol 7 No 1 March 2013 Powder Injection Moulding International Retrieved 1 March 2016 Atkinson H V Davies S December 2000 Fundamental aspects of hot isostatic pressing An overview Metallurgical and Materials Transactions A 31 12 2981 3000 Bibcode 2000MMTA 31 2981A doi 10 1007 s11661 000 0078 2 S2CID 137660703 Gu D D Meiners W Wissenbach K Poprawe R May 2012 Laser additive manufacturing of metallic components materials processes and mechanisms International Materials Reviews 57 3 133 164 Bibcode 2012IMRv 57 133G doi 10 1179 1743280411Y 0000000014 S2CID 137144519 Graybill Benjamin Li Ming Malawey David Ma Chao Alvarado Orozco Juan Manuel Martinez Franco Enrique 18 June 2018 Additive Manufacturing of Nickel Based Superalloys Volume 1 Additive Manufacturing Bio and Sustainable Manufacturing College Station Texas USA American Society of Mechanical Engineers doi 10 1115 MSEC2018 6666 ISBN 978 0 7918 5135 7 S2CID 139639438 Y Tamarin Protective Coatings for Turbine Blades Materials Park OH ASM International 2002 J R Davis ed Handbook of Thermal Spray Technology Materials Park OH The ASM Thermal Spray Society 2004 Boone D H 1986 Physical vapour deposition processes Materials Science and Technology 2 3 220 224 Bibcode 1986MatST 2 220B doi 10 1179 mst 1986 2 3 220 Clarke David R January 2003 Materials selection guidelines for low thermal conductivity thermal barrier coatings Surface and Coatings Technology 163 164 67 74 CiteSeerX 10 1 1 457 1304 doi 10 1016 S0257 8972 02 00593 5 Wadley Research Group University of Virginia Retrieved 3 March 2016 Warnes Bruce Michael January 2003 Improved aluminide MCrAlX coating systems for super alloys using CVD low activity aluminizing Surface and Coatings Technology 163 164 106 111 doi 10 1016 S0257 8972 02 00602 3 Tawancy H M Abbas N M Bennett A December 1994 Role of Y during high temperature oxidation of an M Cr Al Y coating on an Ni base superalloy Surface and Coatings Technology 68 69 10 16 doi 10 1016 0257 8972 94 90130 9 D Chuanxian H Bingtang L Huiling 24 August 1984 Plasma sprayed wear resistant ceramic and cermet coating materials Thin Solid Films 118 4 485 493 Bibcode 1984TSF 118 485C doi 10 1016 0040 6090 84 90277 3 Kawahara Yuuzou January 1997 Development and application of high temperature corrosion resistant materials and coatings for advanced waste to energy plants Materials at High Temperatures 14 3 261 268 Bibcode 1997MaHT 14 261K doi 10 1080 09603409 1997 11689552 Longa Y Takemoto M July 1992 High Temperature Corrosion of Laser Glazed Alloys in Na 2 SO 4 V 2 O 5 Corrosion 48 7 599 607 doi 10 5006 1 3315978 G R Heath P Heimgartner G Irons R Miller S Gustafsson Materials Science Forum 1997 251 54 809 Knotek O 2001 Thermal Spraying and Detonation Gun Processes PDF In Bunshah R F ed Handbook of Hard Coatings Deposition Technologies Properties and Applications Park Ridge NJ Noyes Pub Norwich NY William Andrew Pub pp 77 107 ISBN 9780815514381 Niranatlumpong P Ponton C B Evans H E 2000 The Failure of Protective Oxides on Plasma Sprayed NiCrAlY Overlay Coatings Oxidation of Metals 53 3 4 241 258 doi 10 1023 A 1004549219013 S2CID 136826569 P Fauchais A Vardelle M Vardelle Modelling of Plasma Spraying of Ceramic Films and Coatings Ed Vinenzini Pub Elsevier State Publishers B V 1991 Evans A G Mumm D R Hutchinson J W Meier G H Pettit F S 2001 Mechanisms controlling the durability of thermal barrier coatings Progress in Materials Science 46 5 505 553 doi 10 1016 s0079 6425 00 00020 7 Wright P K Evans A G 1999 Mechanisms governing the performance of thermal barrier coatings Current Opinion in Solid State and Materials Science 4 3 255 265 Bibcode 1999COSSM 4 255W doi 10 1016 s1359 0286 99 00024 8 Wright P K 1998 Influence of cyclic strain on life of a PVD TBC Materials Science and Engineering A245 2 191 200 doi 10 1016 S0921 5093 97 00850 2 Pint B A November 2004 The role of chemical composition on the oxidation performance of aluminide coatings Surface and Coatings Technology 188 189 71 78 doi 10 1016 j surfcoat 2004 08 007 Baufeld B Bartsch M Broz P Schmucker M 2004 Microstructural changes as postmortem temperature indicator in Ni Co Cr Al Y oxidation protection coatings Materials Science and Engineering 384 1 2 162 171 doi 10 1016 j msea 2004 05 052 Nychka J A Clarke D R September 2001 Damage quantification in TBCs by photo stimulated luminescence spectroscopy Surface and Coatings Technology 146 147 110 116 doi 10 1016 S0257 8972 01 01455 4 Mumm D R Evans A G Spitsberg I T 2001 Characterisation of a cyclic displacement instability for a thermally grown oxide in a thermal barrier coating system Acta Materialia 49 12 2329 2340 doi 10 1016 s1359 6454 01 00071 4 Mumm D R Evans A G 2000 On the role of imperfections in the failure of a thermal barrier coating made by electron beam deposition Acta Materialia 48 8 1815 1827 Bibcode 2000AcMat 48 1815M doi 10 1016 s1359 6454 99 00473 5 Gell M Vaidyanathan K Barber B Cheng J Jordan E 1999 Mechanism of spallation in platinum aluminide electron beam physical vapor deposited thermal barrier coatings Metallurgical and Materials Transactions A 30 2 427 435 Bibcode 1999MMTA 30 427G doi 10 1007 s11661 999 0332 1 S2CID 137312835 Evans A G He M Y Hutchinson J W January 2001 Mechanics based scaling laws for the durability of thermal barrier coatings Progress in Materials Science 46 3 4 249 271 doi 10 1016 S0079 6425 00 00007 4 Schulz U Menzebach M Leyens C Yang Y Q September 2001 Influence of substrate material on oxidation behavior and cyclic lifetime of EB PVD TBC systems Surface and Coatings Technology 146 147 117 123 doi 10 1016 S0257 8972 01 01481 5 Chen X Wang R Yao N Evans A G Hutchinson J W Bruce R W July 2003 Foreign object damage in a thermal barrier system mechanisms and simulations Materials Science and Engineering A 352 1 2 221 231 doi 10 1016 S0921 5093 02 00905 X Walston W S 2004 Coating and Surface Technologies for Turbine Airfoils Superalloys 2004 Tenth International Symposium pp 579 588 doi 10 7449 2004 Superalloys 2004 579 588 ISBN 0 87339 576 X Mumm D R Watanabe M Evans A G Pfaendtner J A 2004 The influence of test method on failure mechanisms and durability of a thermal barrier system Acta Materialia 52 5 1123 1131 Bibcode 2004AcMat 52 1123M CiteSeerX 10 1 1 514 3611 doi 10 1016 j actamat 2003 10 045 Brady M P Muralidharan G Leonard D N Haynes J A Weldon R G England R D December 2014 Long Term Oxidation of Candidate Cast Iron and Stainless Steel Exhaust System Alloys from 650 to 800 C in Air with Water Vapor Oxidation of Metals 82 5 6 359 381 doi 10 1007 s11085 014 9496 1 OSTI 1185421 S2CID 136677636 a b c d Blain Loz 10 February 2023 Heat loving lightweight superalloy promises higher turbine efficiency New Atlas Retrieved 12 February 2023 Bibliography edit Levitin Valim 2006 High Temperature Strain of Metals and Alloys Physical Fundamentals WILEY VCH ISBN 978 3 527 31338 9 Shahsavari H A Kokabi A H Nategh S 2007 Effect of preweld microstructure on HAZ liquation cracking of Rene 80 superalloy Materials Science and Technology 23 5 547 555 Bibcode 2007MatST 23 547S doi 10 1179 174328407x179539 S2CID 135755442 External links edit Superalloys Cambridge University Extensive bibliography and links Nickel Based Superalloys Seather The nickel based superalloys guides and links Retrieved from https en wikipedia org w index php title Superalloy amp oldid 1205815569, wikipedia, wiki, book, books, library,

article

, read, download, free, free download, mp3, video, mp4, 3gp, jpg, jpeg, gif, png, picture, music, song, movie, book, game, games.