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1.
The microstructure of martensitic stainless steel powders produced by inert gas atomization was investigated. Depending upon
the powder particle size, the microstructure was found to exhibit a cellular, dendritic, or martensitic morphology. Relationships
between the microstructure scale and the particle diameter were identified. It was found that at a critical particle diameter
of 25 to 30 μm, the structure changed from cellular/dendritic (96.5 vol pct bcc and 3.5 vol pct fcc) to martensite. The solidification
path of the powder particles below and above 25 to 30 μm in size was considered. High-temperature X-ray diffraction (HTXRD) measurements revealed that there is a delay in the appearance
of the fcc phase for the small particle size. The delay in the appearance of the fcc phase is a result of different nucleation
sites for the fcc phase between the large and the small particle size. 相似文献
2.
Thomas F. Kelly Morris Cohen John B. vander Sande 《Metallurgical and Materials Transactions A》1984,15(5):819-833
Individual powder particles of a droplet-processed and rapidly solidified 303 stainless steel are characterized in terms of
microstructure and composition variations within the solidification structure using scanning transmission electron microscopy
(STEM). Fcc is found to be the crystallization phase in powder particles larger than about 70 micron diameter, and bcc is
the crystallization phase in the smaller powder particles. An important difference in partitioning behavior between these
two crystal structures of this alloy is found in that solute elements are more completely trapped in the bcc structures. Massive
solidification of bcc structures is found to produce supersaturated solid solutions which are retained to ambient temperatures
in the smallest powder particles. Calculated liquid-to-crystal nucleation temperatures for fcc and bcc show a tendency for
bcc nucleation at the large liquid supercoolings which are likely to occur in smaller droplets. The importance of small droplet
sizes in rapid solidification processes is stressed.
Formerly with Massachusetts Institute of Technology, Cambridge, MA. 相似文献
3.
R. N. Wright G. E. Korth J. E. Flinn 《Metallurgical and Materials Transactions A》1989,20(11):2449-2457
The nature of interparticle bonding in explosively consolidated, centrifugally atomized (CA), and vacuum gas-atomized (VGA)
Type 304 stainless steel powders has been examined. Stress waves with sufficient amplitude to produce full density do not
necessarily produce metallurgical bonds between particles; the local strain and strain rate are found to determine the degree
of local heating and, in turn, the degree of particle fusion. Particle interaction is found to be limited to nearest neighbors.
The as-consolidated CA material has approximately twice the ultimate tensile strength of mill-annealed wrought Type 304 stainless
steel. Consolidated CA powder has a higher defect density than VGA powder consolidated under the same conditions; however,
the VGA material recrystallizes at a lower temperature due to a lower concentration of carbides. Annealing explosively consolidated
material produced from either powder results in sintering, improved particle bonding, and greater ductility. 相似文献
4.
Abdoul-Aziz Bogno Carlos Riveros Hani Henein Delin Li 《Metallurgical and Materials Transactions B》2016,47(6):3257-3265
This paper investigates amorphous phase formation and rapid solidification characteristics of a CoCr alloy. High cooling rate and high undercooling-induced rapid solidification of the alloy was achieved by impulse atomization in helium atmosphere. Two atomization experiments were carried out to generate powders of a wide size range from liquid CoCr at two different temperatures. Amorphous fraction and kinetic crystallization properties of impulse atomized powders were systematically quantified by means of differential scanning calorimetry. In addition, different but complementary characterization tools were used to analyze the powders microstructures. The fraction of amorphous phase within the investigated powders is found to be promoted by high cooling rate or smaller powder size. The critical cooling rate for amorphous phase formation, which is influenced by the oxygen content in the melt, is found to be ~3 × 104 K s?1 and corresponds to a 160-µm-diameter powder atomized in helium. Hardness of the powders is found to follow a trend that is described by the Hall–Petch relation when a relatively high fraction of crystalline structures is present and decreases with the fraction of amorphous phase. 相似文献
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O. D. Neikov Yu. V. Mil’man A. I. Sirko A. V. Samelyuk A. V. Krainikov N. A. Efimov 《Powder Metallurgy and Metal Ceramics》2007,46(9-10):429-435
The microstructure and mechanical properties of Al-Fe-Ce alloys based on water-atomized powders between 20 and 300 °C are examined in comparison with the properties of similar alloys produced by other rapid crystallization techniques. Changes in atomization parameters vary both the cooling rate (from 104 to 106 K/sec) and powder size distribution (from 5 to 100 µm). The excellent compactability of water-atomized powders facilitates powder consolidation, which is based on hot extrusion and cold pressing of degassed powders. The mechanical properties are examined by tensile tests. The ultimate tensile strength is 500 to 550 MPa at 20 °C and 270 to 300 MPa at 300 °C at adequate plasticity. The properties achieved are comparable with those of similar alloys known from the literature. 相似文献
8.
C. S. Choi W. Sharpe J. Barker R. J. Fields 《Metallurgical and Materials Transactions A》1996,27(4):923-928
Crystallographic properties of an austempered ductile iron (ADI) were studied by using neutron diffraction. A quantitative
phase analysis based on Rietveld refinements revealed three component phases, α-Fe (ferrite), γ-Fe (austenite), and graphite
precipitate, with weight fractions of 66.0, 31.5, and 2.5 pct, respectively. The ferrite phases of the samples were found
to be tetragonal,14/mmm, with ac/a ratio of about 0.993, which is very close to the body-centered cubic (bcc) structure. The austenite phase had C atoms occupying
the octahedral site of the face-centered cubic (fcc) unit cell with about 8 pct occupancy ratio. A strong microstrain broadening
was observed for the two Fe phases of the samples. The particle sizes of the acicular ferrite phase were studied by using
small angle neutron scattering. The analysis suggested a mean rod diameter of 700 A. The scattering invariant predicts a ferrite
volume fraction consistent with the powder diffraction analysis. A textbook case of nodular graphite segregation, with average
diameters ranging from 10 to 20 μm, was observed by optical micrography. 相似文献
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YinG-Yu Chuang Y.Austin Chang Rainer Schmid Jen-Chwen Lin 《Metallurgical and Materials Transactions A》1986,17(8):1361-1372
A generalized approach is proposed to calculate the magnetic contribution to the thermodynamic functions of alloys. This approach
is applied successfully to the Fe-Ni binary system. The predicted magnetic specific heat of the fcc phase at 75 at. Pct Ni
is in agreement with the experimental data within the accuracies of the data and the predicted values. The magnetic contributions
to the Gibbs energies of the fcc and bcc phases for the Fe-Ni alloys obtained from this approach are added to the nonmagnetic
portion of the Gibbs energies. The nonmagnetic portion of the Gibbs energy of the fcc phase is obtained from extensive thermochemical
data at high temperatures as discussed in the paper immediately following this one. The total Gibbs energies of the fcc, bcc,
and the orderedγ′-(FeNi3) phases are then used to calculate/predict phase equilibria of the Fe-Ni binary at temperatures lower than 1200 K. The calculated
equilibria are in agreement with available experimental data. In addition, a irascibility gap of the fcc phase at low temperatures
is predicted, resulting in the formation of a monotectoid equilibrium at 662 K as given below: {fx1361-02} The existence of
the miscibility gap is due to the magnetic Gibbs energy term of the fcc phase which is composition dependent. Experimental
results reported in the literature support the predicted miscibility gap. 相似文献
11.
将硼氢化钠(NaBH4)的水溶液加入到氯化钴(CoCl2·6H2O)和硫酸锆(Zr(SO4)2·4H2O)的混合水溶液中,利用BH-4把混合溶液中的CO2 和Zr4 同时还原出来,首次成功制备出非晶态Co-Zr-B三元纳米合金粉末.用电感耦合等离子体发射光谱(ICP)、X射线衍射(XRD)、选区电子衍射(SAED)、透射电子显微镜(TEM)、差示扫描量热法(DSC)以及振动样品磁强计(VSM)分析了样品的成分、结构和磁性能.发现所制备的不同成分的粉末颗粒呈球形,粒径在20~60nm之间.纳米粉末由非晶相基体和少量晶体相杂质组成,而非晶相基体又由Zr基非晶颗粒和含有Zr的Co基非晶颗粒构成.还原产物中的Co原子和Zr原子的分数之比与金属盐混合溶液中的Co2 与Zr4 离子的分数之比几乎相等.提高NaBH4溶液的加入速度,可增加产物中B元素的含量.样品的晶化温度在765.1~771.3K之间,样品的热稳定性随Zr含量的增加而增加,样品的磁性能也与样品中Co、Zr原子的含量之比有关.当原子数x(Co)/x(Zr)比值从1.94增加到5.14时,饱和磁化强度从4.76emu/g增加到8.87emu/g,矫顽力在1271.66A/m(15.98Oe)到2133.49A/m(26.81Oe)之间不规则变化. 相似文献
12.
Premkumar M. K. Lawley A. Koczak M. J. 《Metallurgical and Materials Transactions A》1992,23(1):3219-3230
Prealloyed rapidly solidified Al-Fe-Ni alloy powder with dispersoid volume fractions of 0.19, 0.25, and 0.32 FeNiAl9 was produced by air atomization. The powder was degassed, canned, and consolidated to full density by vacuum hot pressing and extrusion or by direct extrusion. Microstructures in the alloy powder and consolidated material were characterized by means of optical, scanning (SEM), and transmission electron microscopy (TEM) and constituent phases identified by X-ray diffraction. The coarsening kinetics of the FeNiAl9 dispersoid were moni- tored by differential scanning calorimetry (DSC) and by quantitative metallography. Atomized powders exhibited two scales of microstructures: optically featureless regions and regions with a coarse dispersoid morphology. Within the featureless regions, there are three morphologies, namely, a fine uniform precipitate microstructure, a cellular microstructure, and an eutectic microstructure. The only dispersoid observed in the atomized powders and consolidated material was FeNiAl9). The two scales of microstructure were retained after consolidation, and after hot extrusion, the typical microstructure consisted of a recovered matrix structure with a grain size of 0.2 to 0.3 μm and equiaxed intermetallics of average diameter 0.1 μm. The microstructure was resistant to coarsening up to approximately 370 °C. Coarsening kinetics in this alloy system were consistent with a grain boundary diffusion model (activation energy 146 kJ/mol) and were not appreciably affected by dispersoid volume fraction. 相似文献
13.
Microstructural transitions during containerless processing of undercooled Fe-Ni alloys 总被引:4,自引:0,他引:4
The microstructural development associated with solidification in undercooled Fe-Ni alloys has been reported in different
studies to follow various pathways, with apparent dissimilarities existing as a function of sample size and processing conditions.
In order to identify the possible hierarchy of microstructural pathways and transitions, a systematic evaluation of the microstructural
evolution in undercooled Fe-Ni alloys was performed on uniformly processed samples covering seven orders of magnitude in volume.
At appropriate undercooling levels, alternate solidification pathways become thermodynamically possible and metastable product
structures can result from the operation of competitive solidification kinetics. For thermal history evaluation, a heat flow
analysis was applied and tested with large Fe-Ni alloy particles (1 to 3 mm) to assess undercooling potential. Alloy powders
(10 to 150 μm), with large liquid undercoolings, were studied under the same composition and processing conditions to evaluate
the solidification kinetics and microstructural evolution, including face-centered cubic (fcc)/body centered cubic (bcc) phase
selection and the thermal stability of a retained metastable bcc phase. The identification of microstructural transitions
with controlled variations in sample size and composition during containerless solidification processing was used to develop
a microstructure map which delineates regimes of structural evolutions and provides a unified analysis of experimental observations
in the Fe-Ni system. 相似文献
14.
The phase relationships between the liquid phase and the primary solid phases were investigated in the iron-rich comer of
the Fe-Cr-Ni-C system as part of a larger study of the Fe-Cr-Mn-Ni-C system. The investigation consisted of measurements of
tie-lines for the liquid-delta (bcc) and the liquid-gamma (fcc) equilibria in the iron-rich corner of the Gibbs tetrahedron
bounded by 0 to 25 wt Pct Cr, 0 to 25 wt Pct Ni, and 1.2 wt Pct C (bal. Fe). The temperature ranged from 1811 to 1750 K. Compositions
for the tie-lines were obtained from liquid-solid equilibrium couples and the temperatures of the equilibrium, by differential
thermal analysis (DTA). A mathematical procedure was employed on the experimental data to obtain parameters for a thermodynamic
model of the alloy system. This involved minimization of an error function. The details of this analysis are discussed fully
in this paper. Calculations by the model employing the “best-set” parameters are in good agreement with the experimental results.
The usefulness of the model is demonstrated by calculation of the three-phase equilibrium in the quaternary system as a function
of temperature.
Formerly Research Fellow, Massachusetts Institute of Technology, is Senior Research Engineer, Armco Inc., Middletown, OH 45043 相似文献
15.
采用真空雾化制备了CoCrAlTaY高温合金粉末。结果表明:该合金粉末呈球形,粉末粒度呈近正态分布,粉末由CoAl、γ、Cr27C3和TaC相组成;合金粉末涂层与基体结合良好,其结合力达到52 MPa。 相似文献
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17.
对氩气雾化法制备的高温合金FGH96粉末进行了热等静压(HIP)处理,分析了粉末粒度和氧含量对HIP态合金组织的影响,研究了FGH96合金组织中PPB的类型、相结构和形成机制。结果表明,氩气雾化FGH96粉末的氧含量较低,平均氧含量约为50×10-6,随着粉末粒度降低,颗粒比表面积增大,促进了粉末氧含量的升高;粉末经HIP处理后氧含量具有遗传特征,原始粉末氧含量越高,HIP态合金氧含量也越高,且平均氧含量增至83×10-6;粉末尺寸和氧含量对合金致密化行为无明显影响,HIP态合金密度约为8.33 g·cm-3。小尺寸粉末制备的HIP态合金原始颗粒边界主要析出ZrO2和MC碳化物,而大尺寸粉末制备的HIP态合金原始颗粒边界主要析出大尺寸花瓣状γ’相和少量MC碳化物。粉末粒度和氧含量影响PPB析出,小尺寸粉末因氧含量高经HIP处理时颗粒边界处存在更多、尺寸更大稳定的ZrO2,ZrO2成为MC碳化物析出形核的核心,促进了大量MC碳化物的析出。 相似文献
18.
M. K. Premkumar A. Lawley M. J. Koczak 《Metallurgical and Materials Transactions A》1992,23(12):3219-3230
Prealloyed rapidly solidified Al-Fe-Ni alloy powder with dispersoid volume fractions of 0.19, 0.25, and 0.32 FeNiAl9 was produced by air atomization. The powder was degassed, canned, and consolidated to full density by vacuum hot pressing
and extrusion or by direct extrusion. Microstructures in the alloy powder and consolidated material were characterized by
means of optical, scanning (SEM), and transmission electron microscopy (TEM) and constituent phases identified by X-ray diffraction.
The coarsening kinetics of the FeNiAl9 dispersoid were monitored by differential scanning calorimetry (DSC) and by quantitative metallography. Atomized powders
exhibited two scales of microstructures: optically featureless regions and regions with a coarse dispersoid morphology. Within
the featureless regions, there are three morphologies, namely, a fine uniform precipitate microstructure, a cellular microstructure,
and an eutectic microstructure. The only dispersoid observed in the atomized powders and consolidated material was FeNiAl9. The two scales of microstructure were retained after consolidation, and after hot extrusion, the typical microstructure
consisted of a recovered matrix structure with a grain size of 0.2 to 0.3 μm and equiaxed intermetallics of average diameter
0.1 μm. The microstructure was resistant to coarsening up to approximately 370 °C. Coarsening kinetics in this alloy system
were consistent with a grain boundary diffusion model (activation energy 146 kJ/mol) and were not appreciably affected by
dispersoid volume fraction. 相似文献
19.
The effect of powder particle size on the microstructure, mechanical properties, and fracture behavior of Al-20 wt pct Si
alloy powders was studied in both the gas-atomized and extruded conditions. The microstructure of the as-atomized powders
consisted of fine Si particles and that of the extruded bars showed a homogeneous distribution of fine eutectic Si and primary
Si particles embedded in the Al matrix. The grain size of fcc-Al varied from 150 to 600 nm and the size of the eutectic Si
and primary Si was about 100 to 200 nm in the extruded bars. The room-temperature tensile strength of the alloy with a powder
size <26 μm was 322 MPa, while for the coarser powder (45 to 106 μm), it was 230 MPa. The tensile strength of the extruded
bar from the fine powder (<26 μm) was also higher than that of the Al-20 wt pct Si-3 wt pet Fe (powder size: 60 to 120 μm)
alloys. With decreasing powder size from 45 to 106 μm to <26 μm, the specific wear of all the alloys decreased significantly
at all sliding speeds due to the higher strength achieved by ultrafine-grained constituent phases. The thickness of the deformed
layer of the alloy from the coarse powder (10 μm at 3.5 m/s) was larger on the worm surface in comparison to the bars from
the fine powders (5 μm at 3.5 m/s), attributed to the lower strength of the bars with coarse powders. 相似文献
20.
采用氟盐反应法制备TiB2/Al复合材料铸锭,并以此为原料利用高压气体雾化制粉技术制备TiB2/Al复合材料粉末。利用金相显微镜、扫描电子显微镜、X射线衍射仪、粒度分布仪等手段对所制备铸锭和粉末的组织及性能进行了表征。结果表明:Al熔体中TiB2的溶度积远小于TiAl3和AlB2的溶度积,TiB2自Al熔体中沉淀析出导致的体系Gibbs自由能变化量比TiAl3或AlB2自Al熔体中沉淀析出导致的体系Gibbs自由能变化量的值更小。TiB2/Al复合材料铸锭及粉末均主要由α-Al相和TiB2相组成。气体雾化制备TiB2/Al复合材料粉末中TiB2颗粒具有纳米尺度,且均匀弥散地分布于Al基体之中,不存在明显的偏聚现象。TiB2/Al复合材料粉末的粒度主要分布在10~100 μm之间,呈正态分布,粒径介于10~70 μm粉末占比(质量分数)约为81.1%,粒径大于70 μm粉末收得率为12.6%,粒径小于10 μm粉末收得率为6.3%。 相似文献