Microwave Sintering Of Refractory Metals/alloys: W, Mo,

2y ago
45 Views
2 Downloads
746.97 KB
17 Pages
Last View : 6d ago
Last Download : 3m ago
Upload by : Anton Mixon
Transcription

Journal of Microwave Power and Electromagnetic Energy, 44 (1), 2010, pp. 28-44A Publication of the International Microwave Power InstituteMicrowave Sintering of RefractoryMetals/alloys: W, Mo, Re, W-Cu,W-Ni-Cu and W-Ni-Fe AlloysAvijit Mondal1, Dinesh Agrawal2, Anish Upadhyaya1Department of Materials & Metallurgical EngineeringIndian Institute of Technology, Kanpur 208016, INDIA1Materials Research InstituteThe Pennsylvania State University, University Park, PA 16802, USA2Received: August 5, 2009Accepted: January 28, 2010ABSTRACTRefractory metals and alloys are well known for their high mechanical properties whichmake them useful for wide range of high temperature applications. However, owing to therefractoriness of these metals and alloys, it is very difficult to consolidate them under moderateconditions. Conventional P/M processing is a viable sintering technique for these refractorymetals. One of the constraints in conventional sintering is long residence time which results inundesirable microstructural coarsening. This problem gets further aggravated when using smaller(submicron and nano) precursor powder sizes. Furthermore, conventional heating is mostlyradiative, which leads to non-uniform heating in large components. This review article describesrecent research findings about how these refractory metals and alloys (W, Mo, Re, W-Cu, W-NiCu and W-Ni-Fe) have been successfully consolidated using microwave sintering. A comparativestudy with conventional data has been made. In most cases, microwave sintering resulted in anoverall reduction of sintering time of up to 80%. This sintering time reduction prevents graingrowth substantially providing finer microstructure and as a result better mechanical propertieshave been observed.KEYWORDS: Microwave sintering; Refractory metals/alloys; MicrostruturesINTRODUCTIONRefractory metals are known for their very high melting temperatures. Most refractorymetals used for various applications are tungsten with fusion point of 3420 C, molybdenum of2620 C and rhenium of 3180 C. Because of their high melting point, most refractory metals andalloys are consolidated through powder metallurgy (P/M) techniques, though for some specificapplications mechanical alloying and infiltration technique are also employed. Most commonly,liquid phase sintering (LPS) is used for consolidating tungsten based alloys such as W-Cu, WNi-Cu and W-Ni-Fe compositions [Upadhyaya, 2001]. The LPS offers an advantage of relativelylower sintering temperature, enhanced densification, microstructural homogenization and neartheoretical density.28International Microwave Power Institute

Avijit Mondal et al., Microwave Sintering of Refractory Metals/alloys: W, Mo, Re, W-Cu, W-Ni-Cu and W-Ni-Fe .These refractory metals and alloysoffer a wide range of properties which makethem advantageous for high temperatureapplications over other materials. Sinteredtungsten is an excellent material for manyapplications such as lightings, heating,aerospace, electronic, sports and militaryuses due to its high melting point, highdensity of 19.3 g/cm3, high hardness of 9.75GPa, moderate elastic modulus of 407 GPa,low coefficient of thermal expansion, goodthermal conductivity, and low vapor pressure.Rhenium metal is interesting from a numberof standpoints. It is only second to tungsten,among the metallic elements, in meltingpoint. Its density of 21.0 g/cm3 is higherthan that of tungsten. Annealed material hasexhibited tensile strengths of about 120,000p.s.i. with 25% ductility at room temperature,and it is somewhat harder and more resistantto abrasion than tungsten. Other properties,such as its corrosion resistance and electricalproperties make it promising for incandescentlamp filaments and electrical contacts.Molybdenum is a typical transition metalelement having a high melting point, highmechanical strength, and high modulus ofelasticity. Most of the applications for puremolybdenum metal and its alloys involveas electrodes for electrically heated glassfurnaces and forehearths, nuclear energyapplications, missile and aircraft parts,thermocouple sheaths, flame and corrosionresistant coatings for other metals, and as analloying agent in steel.An important class of tungsten basedmaterial is tungsten heavy alloys (WHA). Atypical tungsten heavy alloy contains 60 to98 wt. % tungsten. The balance is generallya mixture of relatively low melting transitionelements, such as nickel, iron, copper, andcobalt. Due to their unique combinationof properties WHAs have a wide rangeof applications, such as radiation-shield,counter-balanced weights etc.Most important of all applications isits potential to be a replacement of depleteduranium within kinetic energy anti armorpenetrators in ordnance industry. For mostof the applications, near theoretical density,dimensional stability, higher hardness,toughness and very high ductility areimportant.These metals and alloys in conventionalfurnace are sintered at very high temperatures(1500-2000 C) and to avoid thermal shock ata slow heating rate ( 10 C/min) and with anisothermal hold at intermittent temperatures.The high sintering temperature results insignificant microstructural coarsening in thesintered material, leading to the degradationof mechanical properties. This problem isfurther aggravated when the initial powdersize is extremely fine. Hence, it is envisagedthat a sintering method that provides a rapidheating rate, lower sintering temopertaureand duration would mitigate this problem.One of the techniques to achieve rapidand relatively uniform sintering is throughmicrowaves [Rao et al., 1995; Clark andSutton, 1996; Agrawal, 1998].Microwave sintering in the recenttimes has emerged as an innovative techniquefor high temperature material processing.Microwave assisted synthesis is generallyfaster, cleaner and more economical thanthe conventional methods. The possibility ofceramics processing by microwave heatingwas first discussed over 50 years ago by VonHippel [Von Hippel, 1954], and experimentalstudies started in the middle of the 1960s byTinga and co-authors [Tinga et al., 1968; Tingaand Edwards, 1968]. Since then variety ofmaterials such as carbides, nitrides, complexoxides, silicides, zeolieties apatite, etc. havebeen synthesized using microwaves [Bykov et.al., 2001; Booske et al., 1997; Sutton, 1992;Agrawal, 1999; Agrawal et al., 2001; Rodigeret al., 1998; Agrawal et al., 2000].In 1999, for the first time Roy et al.[Roy et al., 1999] reported that a porouspowder metal compact could be heatedand sintered in a microwave field. Theirwork added a new dimension towards theapplication of microwave energy for hightemperature material processing. TheJournal of Microwave Power and Electromagnetic Energy, 44 (1), 2010International Microwave Power Institute29

Avijit Mondal et al., Microwave Sintering of Refractory Metals/alloys: W, Mo, Re, W-Cu, W-Ni-Cu and W-Ni-Fe .results of many investigations in microwavesintering and joining of ceramics, ceramicmetal composites, metals and alloys havebeen reported [Bykov et. al., 2001; Booskeet al., 1997; Sutton, 1992; Agrawal, 1999;Agrawal et al., 2001; Rodiger et al., 1998;Agrawal et al., 2000; Anklekar et al., 2001;Saitou, 2006; Luo, J. et al., 2004; Anklekaret al., 2005; Takayama et. al., 2006; Rybakovet al., 2006; Mishra et al., 2006; Mondalet al., 2008; Mondal et al., 2009]. In themajority of the papers the authors claimacceleration of microwave driven processesas compared with the processes performedusing conventional heating. The accelerationcommonly manifests itself as a reduction in thedensification time of the powder compacts,which is often accompanied by a decrease inthe temperature of sintering. High rates ofvolumetric heating in microwave sintering,not limited by thermal diffusion, preventrecrystallization grain growth and result ina finer and more uniform microstructure inthe sintered bulk materials. It is well knownthat a fine, homogeneous, and fault-freemicrostructure is a necessary prerequisite forenhanced material performance. Similarly,a decrease in the duration of the hightemperature stage leads to reduced graingrowth as a result, to the higher mechanicalstrength in the final product.There are different mechanismsby which microwaves can couple to amaterial and a whole host of ways that themicrowave energy is subsequently absorbedby the system. The main loss mechanisms areelectric, conduction (eddy current), hysteresisand resonance (domain wall and electron spin(FMR)). It is often difficult to ascertain whichloss mechanism, or combination of mechanismsis occurring for a particular material in givenconditions. The different mechanisms dohowever have different dependencies oncertain properties such as sample type andmicrostructure, frequency and temperature.A brief description of these different lossmechanisms for ceramic material can befound in the reference [Clark and Sutton,301996; Agrawal, 1998; Von Hippel, 1954; Tingaet al., 1968; Tinga and Edwards, 1968; Bykovet. al., 2001; Booske et al., 1997; Sutton,1992; Agrawal, 1999; Agrawal et al., 2001;Rodiger et al., 1998; Agrawal et al., 2000].Microwave heating in metals is different fromthat observed in dielectric materials (mostlyceramics). Being good conductors, no internalelectrical field is induced in metals.The induced electrical charge remainsat the surface of a bulk metallic sample. As aconsequence, bulk metals reflect microwavesat room temperature; hence no bulkabsorption (heating) occurs, particularly, attemperatures below 500 C. According to theFaraday’s effect in a conductive material, avarying magnetic field generates an electricfield that gives rise to eddy currents andsubsequently resistive losses. Additionallyduring sintering of particulate metalcompact, each individual powder particle inthe compact is surrounded by a dielectricoxide layer. The presence of such dielectric“shell” on the powder particle prevents theconnectivity percolation between the particlesand increases significantly electromagneticpower that can be absorbed by the compact.In general, the skin depth is relatively smallin metals, since in the microwave regime,the particle sizes are much smaller than thewavelength of microwave radiation; the fieldacross the particle are uniform and causesvolumetric heating. However, for relativelycoarse particle ( 100µm), the heating may beconductive from outside to the interior of thepowder. Recent study confirms that magneticheating plays most important role for metallicmaterials. Quite contrary to the fact thatelectric heating predominates for dielectricmaterials. The detailed microwave absorptionmechanism for metallic material can be foundin the reference already mentioned.From the above discussion it is quiteclear that microwave processing has manyadvantages over conventional methods,especially for sintering applications. Thevarious advantages are: time and energysaving, rapid heating rates, considerablyJournal of Microwave Power and Electromagnetic Energy, 44 (1), 2010International Microwave Power Institute

Avijit Mondal et al., Microwave Sintering of Refractory Metals/alloys: W, Mo, Re, W-Cu, W-Ni-Cu and W-Ni-Fe ialenhancementin reactivity and diffusion kinetics, finehomogeneous microstructures and improvedmechanical properties which lead to betterproduct performance. Microwave-matterinteraction and anisothermal situations oftenproduce better quality and new materials thatare normally not possible with conventionalmethods. These characteristics advantagesof microwave sintering can be exploited toovercome the processing difficulties of therefractory metals and alloys.This review article describes recentresearch findings about how certain refractorymetals and alloys (W, Mo, Re, W-Cu, W-NiCu and W-Ni-Fe) have been successfullyconsolidated using microwave sintering anda comparative study with conventional datahas been made. In most cases, microwavesintering resulted in an overall reduction ofsintering time of up to 80%. This sintering timereduction prevents grain growth providingfiner microstructure and as a result bettermechanical properties have been observed.CONSOLIDATION OF TUNGSTENUsually the consolidation of W powderby conventional heating is difficult andrequires very high temperature (2200 C ormore) in electrical resistance sintering underhydrogen atmosphere. The requirementof excessive high temperature and specialtechnique makes the process more expensiveand imparts a restriction in the sizes andshapes of the sintered products.Low-temperature brittleness is themost crucial aspect in the manufacturing ofpure tungsten metal. Therefore, in the pastmuch effort has been directed at loweringthe ductile to- brittle transition temperature(DBTT) and hence improving the fabricabilityof the metal.The brittleness of polycrystallinetungsten at low temperature is attributed tothe weakness of the grain boundaries, whichleads to initiation of cracking in both wroughtand recrystallized tungsten. Pure, singlecrystalline tungsten (free of grain boundaries)remains ductile down to at least 20K. Anyplastic deformation decreases the transitiontemperature by fining the structure [Lassnerand Schubert, 1999]. The presence of smallamount of interstitial impurities such as O, C,N and H2 has a detrimental effect on DBTT.The solubility for such elements intungsten at room temperature is much lowerwhen compare to high temperature. So duringcooling segregation of such elements at thegrain boundary significantly weakens the grainboundary strength. The ductilizing effectof Re in tungsten have gained outstandingimportance in this regard. Addition of Re cancause the transformation temperature to fallbelow room temperature, even for slightlydeformed products. Many studies have shownthat sintering temperature is related to thepowder size, when the size is in nano-scale,the sintering temperature can be decreasedup to several hundred degrees. The reductionof sintering temperature for nano tungstenhas been reported by several researchers[Sarma and Pabi, 2007; Oda et al., 2006;Bose et al., 2008; Engleman et al., 2008;Johnson, 2008;Wang et al., 2008; Jainet al., 2006; Jain et al., 2006]. The reportedsintering temperature of nano sized tungstenproduced by high energy mechanical millingwas drastically decreased from conventionaltemperature of 2500 C to 1700 C [Malewaret al., 2007]. Researchers have also shownthat pressure assisted process such as sparkplasma sintering [Oda et al., 2006], plasmapressure compaction [Bose et al., 2008],and hot isostatic processing (HIP) [Englemanet al., 2008] etc. helps in further reductionin the processing temperature. Selection ofnano powders over microcrystalline powdershas certain distinct advantages. According tothe literature reported data for both metalsand ceramic nano particles was found to startdensification at temperatures of 0.2–0.4 Tm(Tm - melting temperature) compared to 0.5–0.8 Tm for the conventional powders.It is believed that in the case ofnanostructured powders the grain boundaryJournal of Microwave Power and Electromagnetic Energy, 44 (1), 2010International Microwave Power Institute31

Avijit Mondal et al., Microwave Sintering of Refractory Metals/alloys: W, Mo, Re, W-Cu, W-Ni-Cu and W-Ni-Fe .sliding, dislocation motion, grain rotation,and viscous flow can significantly contributeto the enhanced sintering kinetics [Hahn,1993; Averbach et al., 1996; Bourell andGroza, 1998; Groza, 1999; Groza, 2002].Generally sintering theories hold that thesintering temperature is often correlatedwith melting point of the material. It is longbeen know that the melting temperatureof very fine particles decreases with thesize of the particles [Couchman and Jesser,1977]. Therefore in addition to the fastersintering kinetics, the faster densification innano structured material could be attributedto the lower melting temperature of nanoparticles.In addition to all the above mentionedadvantages, nano tungsten has two distinctadvantages over conventionally sized tungstenpowder. First, the thermal conductivityof nano tungsten is much lower than thatof conventionally sized tungsten powder.Secondly, as in nano dimension grain size areclose to dislocation length, no pinning or pileup of dislocation occurs [Andrey et al., 2004].The contribution of these two phenomenonresults in a material that exhibits a higherpropensity of adiabatic shear, which is veryimportant aspects of this material as a kineticenergy penetrator application is concerned.Wang [Wang et al., 2008] has studied the sizedependent sintering behavior of tungstenpowder.They observed that the startingparticle size before milling plays an importantrole in sinterability of this material, lowerthe size higher will be the sinterability.Although, the final crystallite size aftermilling is same in both the cases. The reasonfor this difference could be attributed withthe difference in particle size after milling.Mohit et al. [Jain et al., 2006] studiedthe application of microwave energy inconsolidating pure tungsten powder. Theyfound 10 to 12% higher sintered density inmicrowave sintering as compare to theirconventional counter part. In another studythey have reported the role of HfO2 and32Y2O3 as successful grain growth inhibitors.They also observed that the introduction ofa secondary oxide (HfO2 and/or Y2O3) had asignificant effect on the powder morphologyand in reducing the primary particle size ofthe as synthesized tungsten powders. Theparticle size was reduced from 350 nm to 80100nm, and the crystallite size was reducedfrom 48 nm to 25 nm with the addition ofdopents [Jain et al., 2006].Prabhu [Prabhu et al., 2008] has alsoinvestigated microwave sintering of puretungsten powder of as received grade andtungsten powder activated by high energymilling (HEM). Their study shows bettersinterability of activated tungsten powder incompare to as received powder.Mondal [Mondal et al., 2009] has alsoreported the similar kind of accelerateddensification in microwave sintered tungstensample. They reported that more than 95%Th density of microwave sintered samplesat 1600 C for 30 min holding in hydrogenatmosphere.Figure 1 describes typical thermalprofile used for their experiments in bothconventional as well as microwave heatingmode.Figure 2 are the SEM micrographof both conventionally and microwaveFigure. 1. Typical thermal profiles of sintered W usingconventional and microwave furnaces [Mondal et al., 2009].Journal of Microwave Power and Electromagnetic Energy, 44 (1), 2010International Microwave Power Institute

Avijit Mondal et al., Microwave Sintering of Refractory Metals/alloys: W, Mo, Re, W-Cu, W-Ni-Cu and W-Ni-Fe .Figure. 2. SEM micrographs of (left) conventional and (rigtj) microwave sintered W at 1600 C for 30 min in H2atmosphere [Mondal et al., 2009].Figure.3. Microwave sintering of complex shaped tungsten samples.sintered samples. Figure 3 show some ofthe commercial pure tungsten products thathave been successfully sintered in microwavefurnace at Penn State’s Microwave ProcessingCenter.CONSOLIDATION OF MOLYBDENUMConventionally the sintering ofmolybdenum powder is conducted using aresistance or induction sintering furnace inan inert atmosphere (argon) or in a reducingatmosphere (hydrogen) [Patrician et al.,1985]. High temperatures in the range of2000 C are employed, resulting in densitiesof 90–95% of theoretical, depending upon thesintering time. Huang [Huang and Hwang,2002] reported the sintering of molybdenumusing vacuum furnaces and obtained densitiesof 97 to 98.5% at a sintering temperature of1750 C with times ranging from 10 to 40 h.Journal of Microwave Power and Electromagnetic Energy, 44 (1), 2010International Microwave Power Institute33

Avijit Mondal et al., Microwave Sintering of Refractory Metals/alloys: W, Mo, Re, W-Cu, W-Ni-Cu and W-Ni-Fe .This also results in abnormal grain growth.Microwave sintering of molybdenum metalpowder has been reported for the first timeby Chillar [Chhillar et al., 2008]. In theirwork, the authors reported sintering of nanomolybdenum powder to obtain submicron grainsize microstructure using microwave energy.As received Mo powder was agglomeratedwith a mean agglomerate size of 1.6 um,but equivalent surface area based on N2adsorption suggests an average particle sizeof 200 nm. Sintering was carried out using theas received powder. Samples with densities ashigh as 98% of theoretical density (TD) wereobtained with limited grain growth in 5 minof sintering time in microwaves, compared to10–20 h in a conventional process.The highlight of this research wasachieving 98%TD in 1 min at 1650 C with asubmicron grain size. Microwave sinteringresult showed that near theoreticaldensities can be obtained at much reducedtemperatures, and with much reducedsintering times, as compared to conventionalsintering.Conventionally sintered samples at1400 C for 10 h resulted in 98%TD. However,using microwave energy 99%TD could beobtained at 1400 C in just 30 min. Thisconclusively shows that microwave sinteringis much faster than conventional sintering.CONSOLIDATION OF RHENIUMArc melting of rhenium in an inertatmosphere or vacuum is possible but themetal produced tends to have coarse grainsize and may have segregation of rheniumoxides at the grain boundaries. These issuesare a problem for further fabrication of aproduct and therefore powder metallurgy hasshown to mitigate some of these problems.Rhenium powder is consolidated using pressuretechniques to a density of approximately 60%of the theoretical density.The pressed compacts are then presintered in a hydrogen atmosphere to facilitatehandling before final sintering. Proper choiceof powder sizes, careful blending and adequate34sintering times and temperatures producebars of high yield and small grain size withthe same homogeneity attainable by electronbeam or arc melting. Subsequent fabricationis performed by swaging, rolling, forging anddrawing with intermediate annealing.Some of these operations may have tobe conducted at elevated temperatures. Theoptimum sequence of these operations variesfor rhenium and it alloys and depends on thefinal end form. Microwave sintering of rheniumpallet has been successfully conducted atPenn State’s microwave processing center.Fig. 4: SEM micrographs of Re pallet in (above) aspressed and (below) microwave sintered at 2000 C for10 min [Mondal et al., 2009].Journal of Microwave Power and Electromagnetic Energy, 44 (1), 2010International Microwave Power Institute

Avijit Mondal et al., Microwave Sintering of Refractory Metals/alloys: W, Mo, Re, W-Cu, W-Ni-Cu and W-Ni-Fe .Relatively high sintered density in the orderof 95% of theoretical has been achieved inmicrowave heating at 2000 C, 20 min soakingtime. Figure 4 shows a SEM micrograph ofas-pressed and microwave sintered rheniumcompact.CONSOLIDATION OF W-CuThere are two ways used to formW–Cu composites: copper infiltration of aporous tungsten skeleton and liquid phasesintering (LPS) of mixed phase compacts. Foreconomical reasons, shape, complexity, andlarge scale production consideration, thelatter technique is the only widely adaptedfabrication routes for W-Cu alloys. However,the lack of solubility between tungsten andcopper makes it very difficult to achieve fulldensification through liquid phase sintering.In the LPS approach, high compactionpressures increase the green density, butresult in increased particle-particle contactsthat limit particle rearrangement duringLPS. Other than rearrangement shrinkage,the sintering shrinkage is due to solid statesintering of the tungsten skeleton, even afterliquid formation. Smaller tungsten powdersinduce faster skeletal sintering or allowfor a lower sintering temperature, which isdesirable since copper evaporation occurs athigh temperatures. The mutual insolubility ofthe W–Cu system denies solution precipitationcontrolled LPS densification. On the otherhand, the addition of small quantities oftransition elements (such as Ni, Co and Fe),activate tungsten skeletal sintering and havea positive impact on the sinterability ofthe W–Cu system. However, these additionsdegrade electrical and thermal conductivity.Higher sintering temperature or longerholding time always help to improve thedensification but copper may diffuse out fromthe skeleton which leads to non homogeneousmicrostructure. Slow heating rate, coreduction of oxides or other thermo chemicalprocesses are all efficient method to improvethe densification of this material. Novelsintering technique has also been explored toenhance W-Cu composite densification whichincludes resistance sintering, plasma sprayingand laser sintering. Microwavesinteringof W-Cu has also been successfully reportedby several researchers [Mondal et al., 2008;Mondal et al., 2009; Mondal et al., 2007].Mondal showed that full densification can beachieved by microwave sintering of W-15Cucomposition. In spite of higher heating rate inmicrowave sintering, cracking in the sinteredsamples was not observed. This is attributedto the volumetric heating nature of microwavesintering. They also reported that microwavesintering lowers the sintering temperatureto achieve the optimum densification aswell as optimum mechanical properties.Figure 5. SEM micrographs of (above) conventional and(below) microwave sintered W-30Cu alloys, sintered at1200 C for 30 min in H2 atmosphere.Journal of Microwave Power and Electromagnetic Energy, 44 (1), 2010International Microwave Power Institute35

Avijit Mondal et al., Microwave Sintering of Refractory Metals/alloys: W, Mo, Re, W-Cu, W-Ni-Cu and W-Ni-Fe .Finer particle size and more homogeneousdistribution of tungsten in the microstructurehave been reported in microwave sintered W15Cu composites. Figure 5 exhibits finer grainsize and homogeneous distribution of boththe phases in microwave and conventionallysintered W-30Cu composites.TUNGSTEN HEAVY ALLOYS (WHAs)Tungsten heavy alloy (WHA) is a groupof two-phase composites, based on W-Ni-Cuand W-Ni-Fe. Price [Price et al., 1938] proposedliquid phase sintering as a viable techniquefor consolidating the W-Ni-Cu alloy. The WNi-Cu system provided an important basis forunderstanding the phenomenology of liquidphase sintering. In fact Cannon [Cannon andLenel, 1953] referred the mechanism of liquidphase sintering as ‘heavy alloy mechanism’.WHA possesses unique combination ofproperties such as high density (16-18 g/cm3), high strength (1000-1700 MPa) and highductility (10-30%).WHAs can be classified into two maingroups based on the binder composition: WNi-Cu and W-Ni-Fe. Besides the high densityand unique combination of high strength andductility, there are other attributes, whichmake WHA a versatile product [Lassner andSchubert, 1999]: The high modulus of elasticityExcellent vibration dampingcharacteristicsIts good machinabilityThe high absorption ability forx-rays and γ-raysGood thermal and electricalconductivitiesLow electrical erosion andwelding tendencyGood corrosion resistanceThe combination of density, ductility,strength, thermal conductivity and corrosionresistance makes them unique in manyapplications such as radiation shields,vibration dampers, kinetic energy penetrators36and heavy-duty electrical contacts. Being astrategic material, all the details regardingthe processing are not available in the openliterature. These alloys are very structuresensitive and therefore a firm understandingof the processing and their physical metallurgyare very critical for attaining better productperformance. In the past, substantialwork has been focused on modifying thematrix composition and post-sintering heattreatment to achieve full densification andoptimal mechanical properties. Residualporosity greater than 0.5% drastically reducesthe mechanical properties, especially thetoughness and ductility.CONSOLIDATION OF W-Ni-Cu ALLOYSIn W-Ni-Cu alloys, normally the nickelto-copper ratio ranges from 3:2 to 4:1. Price[Price et al, 1938] were the first to proposeNi-Cu as the binder for tungsten heavy alloys.They have shown that highly dense W-Ni-Cuheavy alloys could only be obtained by liquidphase sintering.Subsequently, researchers lookedat full densified W-Ni-Cu composites bysolid state sintering. Solid state activatedsintering of tungsten powder with various NiCu additions was studied by Brophy [Brophyet al., 1966]. Their study was mainly confinedto densification mechanism. They proposedthat shrinkage occurs during the initial twostages of sintering: (i) rearrangement and (ii)solution-reprecipitation stages. The role ofphase relationships on the activated sinteringof tungsten was studied by Prill [Prill, 1964].They proposed that at lower Ni:Cu content,the acceleration of sintering of tungstendiminishes. Kothari [Kothari, 1967] studiedthe densification and grain growth kineticsof W-Ni-Cu heavy alloys with different Ni:Curatios.The rate constant for the sinteringprocess was evaluated from the volumechange as a function of sintering period. Theactivation energy was found to be independentof binder composition. Grain growth rate wasproportional to the sintering period. MakarovJournal of Microwave Power and Electromagnetic Energy, 44 (1), 2010International Microwave Power Institute

Avijit Mondal et al., Microwave Sintering of Refractory Metals/alloys: W, Mo, Re, W-Cu, W-Ni-Cu and W-Ni-Fe .[Makarov et al., 1965] studied the coalescencephenomenon in W-Ni-Cu alloys during liquidphase sintering. The effect of tungsten andcopper powder size variation on the sinteredproperties of W-Ni-Cu heavy alloys was carriedout by Srikanth [Srikanth et al., 1983; Srikanthand Upadhyaya, 1984]. They found enhancedsintered properties with finer particle size ofthe constituent with increasing nickel contentin the binder. The effect of composition andsintering temperature on the densificationand microstructure of W-Ni-Cu heavy alloyswas studied by Ramakrishanan [Ramakrishnanand Upadhyaya, 1990]. Kuzmic [Kuzmic, 1966

refractory metals and alloys. This review article describes recent research findings about how certain refractory metals and alloys (W, Mo, Re, W-Cu, W-Ni-Cu and W-Ni-Fe) have been successfully consolidated using microwave sintering and a comparative study with

Related Documents:

ADVANCES IN MODELING OF MICROWAVE SINTERING 12th Seminar Computer Modeling in Microwave Engineering & Applications, Grenoble, France, March 8-9, 2010 32 Combined Microwave-Laser Processing for Sintering of Oxide Ceramics Alexander S. Vanetsev1, Vassily V. Lennikov2 and Xerman de la Fuente Leis2 1Kurnakov Institute of General and Inorganic Chemistry RAS, Moscow, Russia

Metals vs. Non-Metals; Dot Diagrams; Ions Metals versus Non-Metals Dot Diagrams Metals are on the left side. Non-metals on the right. Metals tend to lose electrons. Non-metals gain them tight. Dot Diagrams (sometimes known as Lewis dot diagrams) are a depiction of an atom’s valence elect

Application of Refractory Metals for Corrosion Problems High Corrosion Resistance A good corrosion resistance against molten metals is the prerequisite for a permanent application of die materials in the Found ry Industry. It has already been known for a long time that refractory metals and their alloys show an excellent corrosion resista nce

Refractory Solutions for Aluminium Refractory Installation Refractory Services, as part of the Capital Refractories Ltd group, is here to offer full turnkey solutions for furnace refractory installations. Whatever the job, and whatever the location, or installation, we have a team of exper

The total cost of a refractory is the sum of the cost to purchase the refractory, install the refractory, and maintain the refractory. The patented refractory technology in the WAM AL family of products helps to inhibit the formation of corundum, which extends

Refractory gout is a rare form of severe gout. Both gout and refractory gout are very painful, but refractory gout more often leads to serious problems like permanent joint damage and trouble with moving and walking. Refractory gout may not go away with standard treatments. Other medicines may be needed. P

Metals and Non-metals CHAPTER3 In Class IX you have learnt about various elements.You have seen that elements can be classified as metals or non-metals on the basis of their properties. n Think of some uses of metals and non-metals in your daily life. n What properties did you think of while categorising elements a

time test takers of the American Board of Radiology radiation biology (left), physics (center), and clinical (right) qualifying examinations from 2005-2016 [2017 unavailable]. Reported average pass rates from 2018 are plotted as outliers (for radiation biology and physics) and labeled. Two-sided P-values (with distribution of normality confirmed by the Shapiro test) demonstrate that the .