Intermetallics

In subject area: Materials Science

Intermetallics are compounds formed from two metals that possess distinct crystal structures and properties differing from their parent metals. They typically exhibit long-range orderingwhich can lead to increased strength but reduced ductility and fracture toughness.

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8.1 Introduction

Intermetallics are compounds synthesized either from two metal elements or from one metal and one metalloid with integer ratios (chemometry). Intermetallics have many metallic characteristicssuch as lusterand electrical and thermal conductivity. Intermetallics maintain structural stability even when combined with other chemicalsand appear as ordered solid solutions in phase diagrams.

The chemical formulas of intermetallics formed with the constituent elements A and B will usually be ABA2B and A3B. There are also some special structuressuch as A5B3 or A7B6. The existing A5B3 or A7B6 intermetallics include Mo5Si3Ti5Si3Nb6Fe7 and W6Co7among others.1 Intermetallics can also be formed from three or more constituent elementsso the intermetallic family is very large.

Ordered intermetallic structural materials have recently been the focus of many investigations. Remarkable progress has been made using A3B and AB intermetallics from the Ti–AlNi–Al and Fe–Al systems. Some physical properties of several important intermetallics are listed in Table 8.1.

Table 8.1. Physical properties of several important intermetallics

IntermetallicStructureYoung’s modulus (GPa)Melting point (°C)Orderly critical temperature (°C)Density (g.cm 3)
Ti–AlTi3AlDO19110–145160011004.20
TiAlLI 0176146014603.90
Ni–AlNi3AlL12178139013907.50
NiAlB2293163816385.86
Fe–AlFe3AlDO314015405406.72
FeAlB22591250–14001250–14005.56
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Publisher Summary

The term “intermetallics” is used to designate the intermetallic phases and compounds which result from the combination of various metalsand which form a large class of materials. Intermetallics often have high melting temperatures (usually higher than 1000 C)due partly to the strong bonding between unlike atomswhich is a mixture between metallicionic and covalent to different extents. The presence of these strong bonds also results in high creep resistance. Another factor that contributes to the superior strength of intermetallics at elevated temperature is the high degree of long-range orderwhich results in low diffusivity; the number of atoms per unit cell is large in a material with longrange order. Therefore in alloys in which dislocation climb is rate-controllinga decrease in the diffusion rate would result in a drop in the creep-rate and therefore in an increase of the creep resistance. Creep resistance is a critical property in materials used for high-temperature structural applications. Some intermetallics may have the potential to replace nickel superalloys in parts such as the rotating blades of gas turbines or jet engines due to their higher melting temperatureshigh oxidation and corrosion resistancehigh creep resistanceandin some caseslower density. This chapter reviews the current understanding of creep of intermetallics placing special emphasis on investigations published over the last decade and related to the compounds with potential for structural applications such as titanium aluminidesiron aluminidesand nickel aluminides.

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2023Comprehensive Structural Integrity (Second Edition)Desmond E.P. Klenam... Winston O. Soboyejo

Introduction

Intermetallics are compounds between metals with extremely strong bonding between them resulting in high strength with associated poor ductility due to the strength-toughness trade-offespecially at room temperature (Shabalin2014). Examples of these alloys include Ti3AlTiAlNi3AlNiAlNb3AlNbAlFe3Al and FeAl (Chan and Kim1995; Kastenhuber et al.2017; Kim1992; Soboyejo et al.1997c; Soboyejo et al.2004b,a; Song et al.2017; Srivatsan et al.1995a,b; Wang et al.2017). Intermetallics are desirable for high temperature applications compared to contending ceramics (Soboyejo et al.1997c). This is attributed to their electrical conductivitygood machinability using electro-discharge machining (EDM)easy ways of using conventional joining and non-destructive testing techniqueswhich are mainly applicable to conventional metals (Soboyejo et al.1997c).

Poor ambient temperature toughnessductilityfracture toughness and damage tolerance vary due to poor grain boundary cohesionnegligible slip systems required for deforming polycrystalline materials using the von-Mises criterionlimited cross-slip (exhibiting planar slip) resulting from long range orderpoor twining characteristics and locking of dislocations by impurity atoms (Liu et al.1985; Liu and Stiegler1984; Raj et al.1989; Shabalin2014). High Peierls stresses as associated with long range ordered intermetallics are also contributing factors to the low ductility. The crystal symmetry is lowered while increasing the atomic packing density. This increases frictional stresses impeding dislocations on slip planes. The stoichiometric nature of the alloys contribute to segregations of alloying and trace elements with adverse impact on fracture toughness and ductility (Liu et al.1985; Liu and Stiegler1984). These alloys are susceptible to embrittlement. Fracture toughness at room temperature of selected intermetallics are given in Table 1. Generallya fracture toughness of ~20 MPa√m is the minimum for any conventional design.

Table 1. Fracture toughness of some intermetallics at room or ambient temperature

TypeName of material and processing routeStructureFracture toughness (KIC) MPa√mRefs
Single phaseNiAl [001]
Single crystal
B2
(CsCl)
10(Reuss and Vehoff1991)
NiAl [011]
Single crystal
6
NiAl
Powder metallurgy
2.7–3.8(Kaysser1991)
NiAl
(Extruded ingot)
5.4–5.9(Russel et al.1989)
Ti5Si3D882(Vehoff et al.1993)
MoSi2C11b4–4.6(Soboyejo and Sastry1993)
Al66Ti25Mn9L123.5(Kumar1993)
Al66Ti25Cr93.5
Ti58Al27Nb15DO192.0(Banerjee et al.1993)
Nb3AlA151.1(Murugesh et al.1993)
Multi - phaseNiAl + 5 NbB212.2–15.4(Kaysser1991)
NiAl + 5Ti4.7–14.5
Ti5Si3/Ti3AlD88 + DO1912(Vehoff et al.1993)
TiAl52L10 + DO1910(Deve et al.1992)
TiAl18
(As-extruded)
15(Soboyejo and Sastry1993)
TiAl18/(βTiNb)20
TiAl18
(Arc melting)
30(Tsuyama et al.1992)
Nb3Al/NbA15 +40 vol% Nb6.5(Murugesh et al.1993)
NiAl/TiB2
(Particulate)
B2 + 20 vol% TiB26(Kumar et al.1992)

There is increasing interest in applying ductile phase toughening for the design and engineering of damage tolerant high temperature intermetallics and ceramics (Chan and Kim1995; Kastenhuber et al.2017; Kim1992; Soboyejo et al.1997c; Soboyejo et al.2004b,a; Song et al.2017; Srivatsan et al.1995a,b; Wang et al.2017). Earlier studies were limited to monotonic loading assessments of toughening mechanisms or concepts (Chan19931995; Chan et al.2000; Chan and Kim199219931994; Chan and Shih1998) [11–17]with few experimentations under cyclic loading conditions (Soboyejo et al.1997c). These studies are attributed toughening mechanisms under monotonic loading conditionsplastic stretching of ductile phasescrack deflection and crack bridging mechanisms (Soboyejo et al.1997c).

The current article is divided into six main headings with some subsections. Following the introductionwe will explore the basic mechanisms fatigue in α2 titanium aluminides in Section “Alpha (α2 - Ti3Al) Titanium Aluminides”. This will be followed by Section “Gamma (γ) Titanium Aluminides – Composition and Microstructure” in which we will examine the mechanisms of fatigue in γ-based titanium aluminides while sections “Niobium Aluminides” and “Molybdenum Disilicides” will involve fatigue mechanism in niobium aluminides and molybdenum disilicides respectively. The implications of the observed mechanisms are discussed for the modelling of fatigue in Section “Molybdenum Disilicides”. Conclusions arising from the current review are summarized in Section “Implications”.

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Abstract

The term “intermetallics” has been used to designate the intermetallic phases and compounds that result from the combination of various metalsand which form a large class of materials. There are mainly three types of superlattice structures based on the f.c.c. latticei.e.L12 with a variant of L′12 (in which a small interstitial atom of C or N is inserted at the cube center)L10and L12-derivative long-period structures such as DO22 or DO23. The b.c.c.-type structures are B2 and DO3 or L21. The DO19 structure is one of the most typical superlattices based on h.c.p. symmetry.

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1 Introduction and historical background

There is a demand for materials featuring high strength at temperatures at which conventional heat-resistant materials cannot satisfactorily performfor future aircraft and energy applications. In recent yearsintermetallic compounds with intermediate characteristics between ceramics and metals have attracted attention as structural materials for high temperature service [1]. An intermetallican abbreviated term which has come into universal useis an ordered compound between two or more metalsin simple atomic proportions [2]. The name intermetallic refers to the bonding between the constituent elements of a material system. Specificallythese substances are described to have “mixed bonding”being partially covalentpartially ionicand partially metallic [3]. The crystal structures of intermertallics are different from those of their constituents. This definition includes intermetallic phases and ordered alloys [4]. Intermetallics fall into two large families: weakly ordered (reversible) ones like Cu3Au or CuZn which become disordered on heating before they meltand strongly ordered (permanent) ones like NiAlTiAlor Nb3Al which remain ordered up to the melting temperature [2]. Intermetallics are a fascinating group of materialswhich attract attention from the viewpoints of fundamentals as well as applications [4–6]. For last few decadestremendous world-wide efforts in intermetallics have been seenwhich have largely focused on aluminides with some smaller efforts on silicides. The primary goals were high-temperature or power-generation applicationssuch as aeroengineshigh-temperature edges on aircraft wings and rocket finsautomobile engine valvesturbochargers and so on. Important properties for these applications are the ability to withstand high temperature and aggressive oxidising or corrosive environmentsas well as low specific weight or inertia [7]. Like ceramicshoweverthe greatest disadvantage of intermetallics is their low ductilityparticularly at low and intermediate temperatures. The reasons for the lack of ductility vary from compound to compoundbut include: (1) a limited number of easy deformation modes to satisfy the von Mises criterion(2) operation of dislocations with large slip vectors(3) restricted cross-slip(4) difficulty of transmitting slip across grain boundaries(5) intrinsic grain boundary weakness… etc. [8].

The use of intermetallic compound can be early found in the history. In prehistoric timeshumans used the ordered alloys nature provided (meteoritic Fesingle bondNi for toolsand native Ausingle bondCu for jewellery and fish hooks). Afterwardsfrom ancient to modern-timesalloys compositions and processing techniques were optimized for particular applications without the realization that intermetallic compounds were responsible of such successes [9]. The first ordered intermetallic compound was identified in Russia in 1916by Kumakov and co-workers on the system Ausingle bondCu [10,11]although the concept of long-range order was only clarified by x-ray diffractionin Swedenten years later. Initiallysuch materials were studied only by chemists trying to understand the basis of combination between metals; latermetallurgists began to be interested in their propertiesfirst magnetic ones and later mechanical properties [12]. Serious research on high temperature intermetallics began in the early 1950”'s and increased significantly around 1970 because of their perceived potential in aerospace. With weight saving being a key requirementearly work concentrated on the aluminide intermetallics based on nickel and titanium. Subsequently intermetallics such as Fe3Al have been developed because of their potential benefits in replacing steels in various high temperature applications [13]. Intermetallic-based materials have been exploited in a number of applications not only their mechanical properties but also their chemicalmagneticoptical and semiconducting. The initial references in the literature date of the beginning of last century but the inflexion point was marked by the experiments carried out by Aoki and Izumi [14] who discovered that small additions of boron to Ni3Al improved significantly its poor ductility [15]. According to the studiesthere are estimated about 11,000 distinct binary intermetallic compoundsmost of which are known only through phase diagrams and crystallographic studies but there is no knowledge on the properties they can offer. 500,000 trues ternary intermetallics are calculatedonly 3% of which are known to existand for only an infinitesimally tiny fraction of these do we have any knowledge of their properties. For the likely 10 × 106 quaternary intermetallic compound< 0.01% are even known [9]. Presently they are subject to intensive research in all developed countries around the world. This research is concentrated in universities and specialized research centers particularly in the USACanadaJapanGermanyFrance and Switzerland. The research of these intermetallic alloys is supported particularly by aviation and automobile industry companies [16,17].

Transition metal (TM) intermetallicsespecially TM aluminides like: TiAlNiAlFeAl and Fe3Al have unique propertiese.g.high melting pointsenhanced oxidation resistancerelatively low densityand can be used as soft magnetic materials [18–23]. They have been known and studied since the late nineteenth century. Initiallyinterest in these materials was confined to chemistswho had much difficulty in understanding how metals could combine at all among themselvesoften in several different proportions for the same pairsince this generally seemed to be at variance with elementary notions of valency [24]. Early TM aluminides have fcc-based crystal structure in contrast to the bcc-based crystal structure of late transition metal alloys. Due to the strongly attractive chemical bonding between the bi-metallic speciesthey are ordered and have stoichiometry. Howeverthe energy of interatomic bonds differs from the early TM (TiAlVAl) to the late TM alloys (CoAlNiAl and FeAl) [23]. Conventional processing techniques used to produce intermetallic compounds are generally through a combination of meltingcastingpowder grindingand consolidation by hot pressing. Howeverthese techniques such as melting and casting methods are inapplicable to the fabrication of many intermetallic alloys due tofor examplea large difference between the melting points of constituent elements [25].

For several years mechanical alloying (MA) and mechanical milling (MM) have been known to be a promising route for the processing of structural intermetallics such as iron-nickel- and titanium- aluminides. This is due to many beneficial properties i.e. reliablecheaphigh flexiblility in the selection of synthesis processes and different types of products can be attainedsimplicityeasy to operate and capable of synthesizing explosive materials…etc. [26–28]. The first attempt of producing intermetallics by MA was made by Ivanov [29] for the Alsingle bondNi system. MA is a promising technique to synthesize a variety of equilibrium and nonequilibrium alloy phases starting from blended elemental or prealloyed materials including metalsceramicspolymers and composites. It is a widely used technique that allows the manufacturing of amorphous materialsextended solid solutions, solid solutions of immiscible systemsnanocrystalline materials and quasicrystalline materials. MA is actually a high-energy ball milling process for producing new nanostructured and metastable materials. In this processmechanical energyrather than thermalchemicalelectricor other common forms of energyis used to create phase transformations and chemical reactions at very low temperatures [30]. In MAthe powder particles are trapped between grinding balls and vial wall experiences severe deformationfracture and cold welding. Due to intense deformation and fracture during particle refinement in MAseveral defects such as dislocationsvacancies and stacking faults are induced into the particles resulting increment in free energy of the system [31]. On the other handit has been reported that MA can improve significantly the room temperature ductility of intermetallics because it can achieve: (i) reduction in grain size(ii) disordering of the latticeto improve the dislocation motion (superdislocations do not exist in disordered lattices and therefore only single dislocations need to move for deformation to occur)and (iii) modifying the crystal structure of the phase into a more symmetrice.g.cubic one [31]. The types of intermetallics synthesized by MA include both quasicrystalline and crystalline intermetallic phases. Both equilibrium and metastable phases have been synthesized in the latter category and these also include the disordered and ordered phases [31]. Reasons for the formation of ordered intermetallics have not been investigated in detailit may be assumed that a phase will exist either in the ordered or disordered condition depending upon the balance between atomic disordering introduced by MA and the thermally activated reordering. The reordering is caused by the difference in energy between the ordered and disordered states. Thusif this difference in energy is smallthe alloy will exist in the disordered state whereas if it is large the alloy will be in the ordered state [32]. It has been reported by Eckert et al. [33] that the nature of the phase formed in quasicrystals was different depending on the milling intensity. At very high milling intensitya crystalline intermetallic phase formed while at very low intensityan amorphous phase formed. A quasicrystalline phase formed at intermediate intensities. A number of intermetallics in metallic alloy systems have been synthesized. These include aluminidessilicides and other intermetallics [34]. A novel solid-liquid reaction ball milling technique based on the coupling effect of both mechanochemistry and thermochemistry was developed. Many types of binary intermetallic compound powders were fabricated successfully and most of them are single-phase nanoparticles. Compared with traditional mechanical alloying (MAi.e. high energy ball milling) processesthis mechanochemistry approach shows the advantages in finer particle sizehigher purity of productionfaster reactivity speed and different micro-reaction mechanism. A number of ternary intermetallics of Al-Cu-X (X = FeCoNi) alloy systems such as Al7Cu2FeAl13Cu4Fe3Al65Cu20Fe15Al65Co15Cu20Al69Co25Cu6Al17Cu4Ni and Al0.28Cu0.69Ni have been successfully preparedas reported by Refs [35–38].

It has been long known that partially ordered phases are stronger than those wholly disordered or fully ordered. Thusit is of interest to study the mechanical behavior of materials in various states of partial order [32]. Disordering phenomena of ordered alloys have also been studied to understand the mechanism of disordering and also to produce the disordered material that has a higher ductility/formability than the ordered alloys [33]. Mechanical milling (MM) has emerged as a powerful method of producing disorder in intermetallic alloys. Indeedwhen an ordered intermetallic undergoes heavy deformationone or more of the following polymorphous transformations will occur [39–41]: (a) it will undergo grain refinement down to the nanocrystalline regime(b) chemical long-range order may disappear as signaled by the disappearance of superlattice reflections(c) chemical short-range order (CSRO) may be decreased toward that of a random solid solution [42]CSRO is a measure for the order in the surrounding of an atomi.e.it indicates how strongly neighbouring atoms are correlated(d) the basic topological order and fundamental unit cell of the crystal may change such as in a b.c.c.–f.c.c. transformation [43](e) long-range crystalline topological order may crumble altogether into an amorphous phase [44,45]. The progress of disordering has been monitored by several techniques including X-ray diffraction techniques to measure the lattice parameter and long-range order parametermeasurement of superconducting transition temperature and magnetic susceptibility (if the compound is superconducting in the initial state)Mössbauer techniquesdiffierential scanning calorimetry… etc. [29].

This review is in many aspects different from other papers written on this topic [11,30–32,46]. Indeedas the title indicatesthe current paper emphasizes on the various aspects of synthesis and disordering of B2 TM-Al (TM = FeNiCo) intermetallic alloys by high energy ball milling. A general overview on B2 intermetallics is presentedthen a detailed presentation concerning FeAlNiAl and CoAl intermetallic alloysas well as their properties and synthesis or disordering routesare provided.

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1 Introduction

Intermetallics exhibit the properties of both metals and ceramics and belong to a unique class of materials with an atomic arrangement very different from those of conventionaldisordered alloys. In an intermetallicatoms are bonded together by metallic contributions in addition to covalent/ionic bonds whereas metallic bonds bind the atoms in conventional alloys. Intermetallics CAN exhibit high melting pointslow densitiesexcellent high-temperature strength and high temperature oxidation and corrosion properties. Ancient usage of intermetallics like Cu-Zn for ornamentscoins and as paint colorand Ag-Sn amalgams as dental fillings is well documented [1]. The potential of intermetallics has been widely recognized since the basic theories of bonding and structure of metals and alloys are established around 1930s. Many intermetallics have been developed during the last 80 years for use in critical engineering applications as indicated below:

(1)

shape memory alloys based on NiTi are widely used as part of medical devices and in a variety of civil and defense applications [2];

(2)

permanent and soft magnets based on Ni-Fe (Ni3Fe)Nd-Fe-B (Nd2Fe14B has the highest energy product of commercial magnets)Co-Sm (Co5Sm)and FeCo alloys are used in as diverse applications as automotivetelecommunicationsconsumer electronicsindustrial systemsaerospace industryNMR/MRI body scanners and in surgical tools [3];

(3)

strong super conductors based on Nb-Sn are materials of choice for applications in nuclear magnetic resonance (NMR)magnetic resonance imaging (MRI)linear motor cars and in high-speed trains [4];

(4)

energy storage devices based on Ni metal hydrides for use in civil and defense applications [5];

(5)

Zr3Al as a possible structural material in nuclear reactors due to its resistance to radiation damage [6];

(6)

porous filters of Fe3Al-based alloy for coal refineries [7];

(7)

as Cr-free heating elements of FeAl due to their high electrical resistivity and oxidation resistance [8];

(8)

heat treating trayssteel furnace rollsand forging dies of Ni3Al due to the combination of high strength at high temperatures and excellent oxidation resistance [9];

(9)

TiAl alloys as jet engine turbine blades for the low-pressure section of a commercial aircraft [10];

(10)

MoSi2 and its composites as high temperature structural materialscoatings and as heating elements for furnaces [11]; and

(11)

Ti-Si in microelectronic applications [12].

While the above list is not exhaustivethe scientific and engineering pursuit of intermetallics is critical to civiltransportelectronicdefense and national security in addition to being a fascinating field of science for materials engineersaerospace engineerschemists and physicists. Intermetallic based permanent and soft magnetic materials [3,13,14] are also of economic importanceand their market size alone accounts for at least several billion dollars in 2016 [13,14].

Of the various intermetallic compoundsaluminides of transition metals FeNiTiCoand Nb have received most of the attention. Of thoseiron aluminides based on Fe3Al and FeAl exhibit attractive properties as compared to steels and superalloys as indicated below [7–8,15–23]:

1.

lower densities than that of many stainless steelsand offer better strength-to-weight ratio’s;

2.

higher Al content (in the range of 15–30 wt% depending on the intermetallic) as compared to Al content of 6 wt% or less in steels and superalloys;

3.

excellent oxidation resistance even at 1000 °C;

4.

better corrosion resistance in oxidizing and reducing environments;

5.

ability to either reduce or eliminate the need of strategic elements such as Cr as an alloying element;

6.

ability to match thermal expansion properties to majority of the steels;

7.

use as heating elements due to high electrical resistivity that increases with temperature; and

8.

good corrosion resistance in many aqueous environments.

Single crystals of intermetallic alloys are ductilebut unfortunatelymany intermetallics in polycrystalline form are brittle at room temperaturedue to grain-boundary weaknessrestricted cross slipdifficulty in twinningand a lack of dislocation movement due to impurities. In additionthe brittleness in Ni3AlFe3Aland FeAl arises from an extrinsic environmental effect that can be overcome by alloyingmicrostructural controlor coating [9,15,16,24–26]. An understanding into the brittle nature of ordered intermetallic alloys led to successful microalloying and macroalloying to significantly improve the ductilitymicrostructuremechanical properties and fabricability of intermetallic alloys. Several articles in special symposia and reviews describe the underlying principles to improve the physical propertiesductilitymechanical propertiesand processing of intermetallic alloys [9,15,16,18,20,22–27]. They are based on controlling the symmetry of the crystal structureengineering grain boundary structure and chemistryoptimization of microstructureelimination of hydrogen induced cracking in Ni3AlFe3Aland FeAl due to interaction of Al with moistureand control of phase stability. Alloys based on iron and nickel aluminides exhibit excellent resistance to high temperature corrosion in aggressive atmosphereseven when the partial pressure of oxygen is lowdue to the formation of a protective surface layer of alumina. The high-temperature oxidation and corrosion resistanceparticularly of Ni3AlNiAlFe3Al and FeAl alloysis due to the high Al content of the alloys (Table 1)and Table 2 provides attributes of some selected intermetallic compounds and their maximum use temperatures [9]. In contrastalmost 98% of alloys and superalloys capable of operating above 700 °C in oxygen environments contain as high as 18 wt% of Cr and less than 2 wt% Al. Alloys containing chromium form Cr2O3 on exposure to air or oxygenand the dissociation of Cr2O3 to CrO3 limits their oxidation resistance to 950 °C. On the other handnickel and iron aluminides provide excellent corrosion resistance beyond 950 °C owing to their high aluminum contents and high melting points [7,9,15,16,19–23].

Table 1. Heats of formationaluminum contentsand melting points of selected intermetallics.

IntermetallicHeat of formationa ΔHf298 (kcal/mole)Alwt.%Melting point°C
Nickel base
Ni3Al–36.6 ± 1.213.281395
NiAl–28.3 ± 1.231.491639
Ni2Al3–67.5 ± 4.040.811133
NiAl3–36.0 ± 2.057.96854

Iron base
Fe3Al–16.013.871502
FeAl–12.032.571215
FeAl2–18.949.101164
Fe2Al5–34.354.701171

From Ref. [20].

a
From selected values of the Thermodynamic Properties of Binary Alloyseds R. HultgrenP. D. DesaiD. T. HawkinsM. Gleiser &amp; K. K. KelleyAmerican Society of MetalsMaterials ParkOhio1973; and 0. Kubachewski and C. B. AlcockMetallurgical ThermochemistryStudent EditionPergamon PressNew York1979.

Table 2. Attributes and upper-use temperature limit for selected intermetallic compounds.

Empty CellEmpty CellMaximum use temperature°C
IntermetallicPropertyStrength limitCorrosion limit
Ni3AlOxidationcarburizationand nitridation resistance; high temperature strength11001150
NiAlHigh melting point; high thermal conductivity; oxidationcarburizationand nitridation resistance12001400
Fe3AlOxidation and sulfidation resistance7001200
TiAlLow density is the real advantage; good specific-strength properties and wear resistance1000800
Ti3AlLow density; good specific strength760650
Ni3SiOxidation and reducing environment resistance; good resistance in sea water and sulfuric acid; good resistance in ammonia reactor up to 900 °C8001000
FeAlOxidationsulfidationmolten saltand carburization resistance8001200
MoSi2High melting point; excellent resistance to oxidation; exhibits metallic conductivity13001600

From Ref. [9].

This review presents a brief summary on (a) the development of ductile iron aluminides and their mechanical properties(b) unique wear resistance properties of aluminides and their composites(c) the excellent oxidation and corrosion resistant properties(d) microstructure and the properties of iron aluminide coatings made by plasma sprayHVOF and cold spray techniques(e) status on spray forming of iron aluminide foilsand (f) the promise and the prognosis of aluminide utilization for industrial applications.

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1 Introduction

The term “intermetallics” has been used to designate the intermetallic phases and compounds that result from the combination of various metalsand which form a large class of materials [592]. There are mainly three types of superlattice structures based on the f.c.c. latticei.e.L12 with a variant of L′12 (in which a small interstitial atom of C or N is inserted at the cube center)L10and L12-derivative long-period structures such as DO22 or DO23. The b.c.c.-type structures are B2 and DO3 or L21. The DO19 structure is one of the most typical superlattices based on h.c.p. symmetry. Table 6 lists the crystal structurelattice parameterand density of selected intermetallic compounds [593]. A comprehensive review on the physical metallurgy and processing of intermetallics can be found in Ref. [594].

Table 6. Crystal structurelattice parametersand density of selected intermetallic compounds

AlloyStructure (Bravais lattice)Lattice parametersDensity (g cm−3)
a (nm)c (nm)
Ni3AlL12 (simple cubic)0.3577.40
NiAlB2 (simple cubic)0.2885.96
Ni2AlTiDO30.5856.38
Ti3AlDO190.5770.4644.23
TiAlL100.3980.4053.89
Al3TiDO220.3950.8603.36
FeAlB2 (simple cubic)5.4–6.7 [599]
Fe3AlDO35.4–6.7 [599]
MoSi2C11b6.3

Intermetallics often have high melting temperatures (usually higher than 1000 °C)due partly to the strong bonding between unlike atomswhich isin generala mixture between metallicionicand covalent to different extents. The presence of these strong bonds is also associated with high creep resistance. Another factor that contributes to the superior strength of intermetallics at elevated temperature is the high degree of long-range order [596]which results in low diffusivity; the number of atoms per unit cell is large in a material with long-range order. Thereforein alloys in which dislocation climb is rate-controllinga decrease in the diffusion rate would result in a drop in the creep rate and therefore an increase of the creep resistance.

One major disadvantage of these materialswhich is limiting their industrial applicationis low fracture toughness [597]. This is attributed to several factors. Firstthe strong atomic bonds as well as the long-range order give rise to high Peierls stresses. Secondgrain boundaries are intrinsically weak. The low boundary cohesion results in part from the directionality of the distribution of the electronic charge in ordered alloys [594]. The strong atomic bonding between the two main alloy constituents is related to the p-d orbital hibridizationwhich leads to a strong directionality in the charge distribution. The directionality is reduced in grain boundaries and the bonding becomes much weaker. Other factors that may contribute to the brittleness in intermetallics are the limited number of operative slip systemssegregation of impurities at grain boundariesa high-work hardening rateplanar slipand the presence of constitutional defects. The latter may befor exampleatoms occupying sites of a sublattice other than their own sublattice (antisites) or vacancies of deficient atomic species (constitutional vacancies). The planar faultsdislocation dissociationsand dislocation core structures typical of intermetallics were summarized by Yamaguchi and Umakoshi [598]. Other so-called extrinsic factors that cause brittleness are the presence of segregantsinterstitialsmoisture in the environmentpoor surface finishand hydrogen [599]. It appears that those intermetallics with more potential as high-temperature structural materialsi.e.those that are less brittleare compounds with high crystal symmetry and small unit cells. Thusnickel aluminidestitanium aluminidesand iron aluminides have been most studied over the last few decades. These investigations were stimulated by both the possibility of industrial application and scientific interest [592–601][592][593][594][595][596][597][598][599][600][601].

Creep resistance is a critical property in materials used for high-temperature structural applications. Some intermetallics may have the potential to replace nickel superalloys in parts such as the rotating blades of gas turbines or jet engines [602] due to their higher melting temperatureshigh oxidation and corrosion resistancehigh creep resistanceand in some cases lower density. The creep behavior of intermetallics is more complicated than that of pure metals and disordered solid solution alloys due to their complex structures together with the varieties of chemical composition [23,603][23][603]. The rate-controlling mechanisms are still not fully understood despite significant efforts over the last couple of decades [592,598,604–612][592][598][604][605][606][607][608][609][610][611][612].

In the followingthe current understanding of creep of intermetallics will be reviewedplacing special emphasis on investigations published over the last two decades and related to the compounds with potential for structural applications such as titanium aluminidesiron aluminidesand nickel aluminides.

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2023Comprehensive Structural Integrity (Second Edition)Desmond E.P. Klenam... Winston O. Soboyejo

Key Points

Intermetallics are compound formed between metals with poor fracture toughness and ductility due to strong dependence on stoichiometrysegregation of alloying and trace elementslimited slip systems restricting cross slips.

Improvement in ductility and fracture toughness are achieved through macro and micro-alloying coupled with tailoring the heat treatment to induce the required microstructure.

Toughening mechanisms in intermetallics are mainly by intrinsic and extrinsic approaches – intrinsic toughening is ahead of the crack tip mainly by damaged associated with microstructural featureswhereas extrinsic toughening occurs behind the tip of the cracksreducing the driving force of the crack propagation.

Intrinsic toughening generally occurring in metals is associated with resharpening and blunting of cracks under cyclic conditions. Extrinsic toughening generates inelastic zones about the crack from slidingwedgingand bridging.

Intermetallics and ceramics are inclined to fatigue crack growth from the deterioration of the crack shielding effects during cyclic loading.

Alloying of Nb-based intermetallic and volume of the intermetallic phase is critical to inducing significant toughening.

Pronounced toughening of molybdenum disilicides is through the introducing of ductile phases in the form of whiskers and fibers.

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2019Progress in Solid State ChemistryAyesha Khan Tareen... Minghui Yang

2.1 Intermetallic nitrides

Intermetallic nitrides has dominant metal-metal (M-M) bonding and interstitial N atoms are between metals atoms [59]. An intermetallic (intermetallic alloy/compound) is one with solid-state compound ordered crystal structurewhich exhibits well defined stoichiometry. G. E. R. Schulze in 1967 [60] explained “intermetallic compounds” as solid phases containing two or more metallic elementswith optionally one or more non-metallic elementswhose crystal structure differs from that of the other constituents. They have generally high melting points and are brittle in nature. They usually offer tuning between metallic and ceramic properties. For instance choices may be made to achieve resistance or hardness at elevated temperatures. They can also exhibit chemicalsuperconductingand magnetic properties because of their strong internal ordered atoms. They are used for hydrogen storage [42]electron storage for electrochemical analysis [61] and hard enough to use as cutting tools [62].

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1999Modern Physical Metallurgy and Materials Engineering (Sixth Edition)R.E. Smallman CBEDScFRSFREngFIMR.J. Bishop PhDCEngMIM

9.6.1 General properties of intermetallic compounds

In terms of their propertiesintermetallic compounds are generally regarded as a class of materials between metals and ceramics which arises from the bonding being a mixture of metallic and covalent. Intermetallics are intrinsically strong (and in the Ll2-ordered fcc compounds increases with temperature up to about 600°C) with high elastic modulus. The strong bonding and ordered structure also gives rise to lower self-diffusion coefficients and hence greater stability of diffusion-controlled properties. Some of the compounds of current interest are shown in Table 9.4. Intermetallics containing aluminium or silicon exhibit a resistance to oxidation and corrosion because of their adherent surface oxides. Those based on light elements have attractive low density giving rise to high specific properties particularly important in weight-saving applications.

Table 9.4. Comparison of physical properties of some intermetallic compounds

CompoundCrystal structureMelting temp. (°C)Density (kg m−3)Young's modulus/density
Ni3AlLl2 (ordered fcc)1400750045
Ni3SiLl2 (ordered fcc)11407300
NiAlB2 (ordered bcc1640586035
Ti3SiD019 (ordered cph)1600420050
TiAlLl0 (ordered tetragonal)1460391024
FeAlB2 (ordered bcc)1300556047

Like ceramicshoweverthe greatest disadvantage of intermetallics is their low ductilityparticularly at low and intermediate temperatures. The reasons for the lack of ductility vary from compound to compound but include (1) a limited number of easy deformation modes to satisfy the von Mises criterion(2) operation of dislocations with large slip vectors(3) restricted cross-slip(4) difficulty of transmitting slip across grain boundaries(5) intrinsic grain boundary weakness(6) segregation of deleterious solutes to grain boundaries(7) covalent bonding and high Peierls-Nabarro stress and (8) environmental susceptibility. It has been demonstratedhoweverthat some intermetallics can be ductilized by small alloying additions: Ni3Al with boronTiAl with MnTi3Al with Nb. This observation has encouraged recent research and development of intermetallics and the possibility of application of those materials.

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