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1.
通过射频等离子体球化处理工艺,以不规则形状钨粉为原料,制备了球形钨粉,并研究了加料速率和粉末粒度对粉末球化率的影响。采用扫描电子显微镜、X射线衍射和激光粒度分析仪对球化处理前后粉末的形貌、物相和粒度分布进行了测试和分析。结果表明:粒度在5.5~26.5 μm范围的不规则形状钨粉,经等离子球化处理后得到表面光滑、分散性好、球化率可达100%的球形钨粉。球化处理后,粉末的粒度略微增大。随加料速率的增加,钨粉的球化率降低。随着钨粉球化率的提高,粉末的松装密度和流动性得到显著改善。松装密度由6.80 g/cm3 提高到11.5 g/cm3,粉末流动性由14.12 s/50 g提高为6.95 s/50 g  相似文献   

2.
以不规则形的钕铁硼粉为原料,使用射频等离子体球化处理工艺,制备球形钕铁硼粉.研究了原料的加料速率和粉末粒度对粉末球化率的影响.通过扫描电子显微镜观察对比了等离子球化处理前后粉末及截面形貌,采用X射线衍射方法测试分析了球化过程中氧化物的生成.检测了球化前后粉末的松装密度及其粒度分布.结果表明:不规则形状的钕铁硼粉经等离子球化处理后其球化率可达到100%,松装密度由2.778 g/cm3提高到3.785 g/cm3,粉末流动性由43.3 s/50 g提高到27.5 s/50 g.该粉末适用于凝胶注膜成型及注射成型.  相似文献   

3.
以不规则状钠还原钽粉为原料,采用射频等离子体球化技术制备高纯致密球形钽粉,实现了还原钽粉的球化、致密化和纯化。研究了送粉速率、载气流量、反应室压力等工艺参数对钽粉球化率及粉体特性的影响,并探索了球化钽粉的选区激光熔化成形适用性。结果表明:不规则状钠还原钽粉,经射频等离子体球化处理后可得到表面光滑、内部致密、高纯低氧、球化率可达100%的球形钽粉。球化处理后,钽粉粒度分布变窄。钽粉的球化率随送粉速率的增大而降低,随载气流量的增加先升高后降低。弱负压更有利于获得较高球化率的钽粉。随着球化率的提高,钽粉的流动性能显著改善,松装密度与振实密度明显提高。当送粉速率为30 g/min,载气流量为5.0 L/min,反应室压力为82.7 kPa时,球形钽粉霍尔流速提高到5.98 s/50g,与不规则形钠还原钽粉相比,松装密度由3.503 g/cm~3提高到9.463 g/cm~3,振实密度由5.344g/cm~3提高到10.433g/cm~3,且氧含量由0.076%降低至0.0481%。另外,射频等离子体球化钽粉具有良好的选区激光熔化成形适用性,其试样致密度ρ≥99.5%,抗拉强度σ_b=693 MPa,屈服强度σ_(0.2)=616 MPa,延伸率δ=28.5%。  相似文献   

4.
研究了原料钼粉携带气体流量和钼粉加料速率对感应等离子球化钼粉形貌和粒度的影响。球化前后钼粉的微观形貌用扫描电镜(SEM)观测,粉体物相用X射线衍射仪(XRD)分析,等离子体处理前后钼粉的松装密度和振实密度分别用斯科特容量计和振实密度仪检测。结果表明,等离子体处理后产品仍为纯金属钼粉,形状由不规则变为球形,颗粒平均粒径由原料的40~70 μm减小至35~60 μm,振实密度由2.5 g/cm3提高到5.8 g/cm3。制备球形钼粉最佳工艺参数为:加料速率45 g/min,携带气体流量0.6 m3/h。感应等离子体是制备高纯致密球形钼粉的有效技术。  相似文献   

5.
球形钨粉以其良好的流动性、高的松装密度和振实密度广泛应用于喷涂、增材制造等材料制备领域。本文以不规则形状钨粉颗粒为原料,采用射频等离子球化技术制备球形钨粉,并对球形钨粉进行铺粉及成形实验效果评价。在射频等离子球化过程中,研究球化工艺参数(送粉速率、送粉位置)和原料粉末形态对球化结果的影响。在铺粉实验方面,研究粉末特征和铺粉层厚对铺粉效果的影响。采用扫描电子显微镜、激光粒度分析仪和BT-100粉体综合特性测试仪对球化处理前后粉末的形貌、粒度、流动性、松装密度和振实密度进行测试和分析。结果表明:经过球化处理后,钨粉颗粒呈规则球形,表面光滑,球化率可达100%,流动性、松装密度和振实密度得到明显提高。球化率高的粉末流动性好,铺粉效果好;随着层厚的增加,铺粉效果逐渐得到改善;采用合适粒径的球形钨粉打印的钨薄壁件表面相对光洁,尺寸精度高。  相似文献   

6.
采用直流电弧热等离子体对不规则TA1粉末进行球化处理。利用金相显微镜、扫描电子显微镜、粒度粒形分析仪、霍尔流速计、斯科特容量计及氧氮分析仪等分析测试手段,研究球化工艺对粉末组织形貌、粒度分布、球形度、流动性、松装密度及氧含量的影响。结果表明,球化处理可将不规则形状TA1粉末球化为表面附着亚微米颗粒的实心球形;球形粉末内部组织由等轴状α相转变为长条状α相。球化处理使TA1粉末平均粒径和氧含量降低,球形度升高。原料粉末粒度越小、等离子体发生器功率越高,球化后粉末平均粒径越小,球形度越高;但会导致球化后粉末中亚微米颗粒含量增加、粉末流动性变差、松装密度降低;去除亚微米颗粒可以提高粉末流动性,并进一步降低氧含量。  相似文献   

7.
以不规则状钠还原钽粉为原料,采用射频等离子体球化技术制备高纯致密球形钽粉,实现了还原钽粉的球化、致密化和纯化。研究了送粉速率、载气流量、反应室压力等工艺参数对钽粉球化率及粉体特性的影响,并探索了球化钽粉的选区激光熔化成形适用性。结果表明:不规则状钠还原钽粉,经射频等离子体球化处理后可得到表面光滑、内部致密、高纯低氧、球化率可达100%的球形钽粉。球化处理后,钽粉粒度分布变窄。钽粉的球化率随送粉速率的增大而降低,随载气流量的增加先升高后减小。弱负压更有利于获得较高球化率的钽粉。随着球化率的提高,钽粉的流动性能显著改善,松装密度与振实密度明显提高。当送粉速率为30g/min,载气流量为5.0slpm,反应室压力为12.0Psi时,球形钽粉霍尔流速提高到5.98s/50g,松装密度由3.503g/cm3提高到9.463g/cm3,振实密度由5.344g/cm3提高到10.433g/cm3,且氧含量由0.076%降低至0.0481%。另外,射频等离子体球化钽粉具有良好的选区激光熔化成形适用性,其试样致密度ρ≥99.5%,抗拉强度σb=693MPa,屈服强度σ0.2=616MPa,延伸率δ=28.5%。  相似文献   

8.
采用射频等离子体法制备了高度球形化的TC4(Ti6Al4V)合金粉末。主要探究仪器送粉喷嘴高度、产生等离子体的功率、反应室的压力、原料粉体的粒度分布、送粉速率以及载气的气流速率等对于粉体球化率的影响。通过SEM图像观察粉体的形貌变化并计算粉体的球化率,利用XRD图谱测定球化前后粉体相结构。结果表明,通过观察球化粉末横截面可知粉末为实心球体且表面光滑,球化后粉末流动性明显提高,松装密度增大,粒度分布变窄,适合3D打印等应用技术对于合金粉体的要求。实验中,调节送粉喷嘴高度为12.5 cm,反应室压力为101.36 kPa,送粉速率为1.742 g/min,产生等离子气的功率为27.2 kW且控制原料粉体的粒度分布在38~63μm时,可使得球化率达到99%,明显高于其他球化粉末制备方法。  相似文献   

9.
采用等离子体球化处理和放电等离子烧结(SPS)相结合的方法制备了钡钨阴极多孔钨基体。研究了等离子体球化处理工艺参数对钨粉的球化率和性能的影响规律,以及SPS制备的多孔钨基体的微观组织和相应钡钨阴极的发射性能。结果表明:当喂粉速率和载气流量分别为2.4 g/min和4.0 L/min时,可得到球化率大于98%,且表面光滑、球形度高的球形钨粉;经球化处理后,钨粉的松装密度和流动性显著提高。与原料钨粉相比,采用球形钨粉制备得到的多孔钨基体的孔隙结构和分布均得到显著改善,且开孔率由18.3%提高至19.7%;相应的钡钨阴极在1050℃下的饱和脉冲发射电流密度由8.7 A/cm~2提高至11.2 A/cm~2。  相似文献   

10.
探究了使用大气等离子喷涂设备制备适合热喷涂使用的球形CaF2/BaF2共晶粉末的可能性。68%BaF2、32%CaF2粉末(质量分数)经过1 100℃真空烧结后,形成致密的块状氟化物共晶。机械破碎后的氟化物共晶经过等离子焰流重熔后得到了球形的氟化物共晶。使用F14-1流动性和松装密度测定仪测量球化前后粉末的流动性和松装密度。采用扫描电子显微镜,XRD表征球化前后粉末的形貌和物相组成。结果表明:球化后的粉末呈现较好的球形,球化后粉末的流动性和松装密度较球化前也有较大的改善:球化后共晶粉末的流动时间为55.20s/50g,松装密度为1.89g/cm3;另外,球化后共晶粉末还表现出良好的高温润滑性能:含有10%CaF2/BaF2共晶(质量分数)的镍基涂层在600℃和800℃的平均摩擦因数都小于0.3。  相似文献   

11.
In as-welded state, each region of 2219 aluminum alloy TIG-welded joint shows diff erent microstructure and microhardness due to the diff erent welding heat cycles and the resulting evolution of second phases. After the post-weld heat treatment, both the amount and the size of the eutectic structure or θ phases decreased. Correspondingly, both the Cu content in α-Al matrix and the microhardness increased to a similar level in each region of the joint, and the tensile strength of the entire joint was greatly improved. Post-weld heat treatment played the role of solid solution strengthening and aging strengthening. After the post-weld heat treatment, the weld performance became similar to other regions, but weld reinforcements lost their reinforcing eff ect on the weld and their existence was more of an adverse eff ect. The joint without weld reinforcements after the post-weld heat treatment had the optimal tensile properties, and the specimens randomly crack in the weld zone.  相似文献   

12.
After nearly two years' tense construction, the first phase of industrialized base of Shenyang Research Institute of Foundry (SRIF), located at the Tiexi Casting and Forging Industrial Park in the west of Tiexi District, has now been completed and formally put into operation.  相似文献   

13.
Institute of Process Engineering, Chinese Academy of Sciences, China, has proposed a method for oxidative leaching of chromite with potassium hydroxide. Understanding the mechanism of chromite decomposition, especially in the potassium hydroxide fusion, is important for the optimization of the operating parameters of the oxidative leaching process. A traditional thermodynamic method is proposed and the thermal decomposition and the reaction decomposition during the oxidative leaching of chromite with KOH and oxygen is discussed, which suggests that chromite is mainly destroyed by reactions with KOH and oxygen. Meanwhile, equilibrium of the main reactions of the above process was calculated at different temperatures and oxygen partial pressures. The stable zones of productions, namely, K2CrO4 and Fe2O3, increase with the decrease of temperature, which indicates that higher temperature is not beneficial to thermodynamic reactions. In addition, a comparison of the general alkali methods is carried out, and it is concluded that the KOH leaching process is thermodynamically superior to the conventional chromate production process.  相似文献   

14.
The effect of isochronal heat treatments for 1h on variation of damping, hardness and microstructural change of the magnesium wrought alloy AZ61 was investigated. Damping and hardness behaviour could be attributed to the evolution of precipitation process. The influence of precipitation on damping behaviour was explained in the framework of the dislocation string model of Granato and Lücke.  相似文献   

15.
The motion of melt droplets in spray degassing process was analyzed theoretically. The height of the treatment tank in spray degassing process could be determined by the results of theoretical calculation of motion of melt droplets. To know whether the melt droplets would solidify during spraying process, the balance temperature of melt droplets was also theoretically analyzed. Then proof experiments for theoretical results about temperature of melt droplets were carried. In comparison, the experimental results were nearly similar to the calculation results.  相似文献   

16.
On the basis of the single-particle framework, a new theory on inclusion growth in metallurgical melts is developed to study the kinetics of inclusion growth on account of reaction and collision. The studies show that the early growth of inclusion depends on reaction growth and Brawnian motion collision, and where the former is decisive, the late growth depends on turbulence collision and Stokes' collision, and where the former is dominant; collision growth is very quick during the smelting process, lessened in the refining process, but nearly negligible in the continuous casting process.  相似文献   

17.
An approach based on film buckling under simple uniaxial tensile testing was utilized in this paper to quantitatively estimate the interfacial energy of the nanostructured multilayer films(NMFs) adherent to flexible substrates. The interfacial energies of polyimide-supported NMFs are determined to be *5.0 J/m2 for Cu/Cr, *4.1 J/m2 for Cu/Ta,*2.8 J/m2 for Cu/Mo, *1.1 J/m2 for Cu/Nb, and *1.2 J/m2 for Cu/Zr NMFs. Furthermore, a linear relationship between the adhesion energy and the interfacial shear strength is clearly demonstrated for the Cu-based NMFs, which is highly indicative of the applicability and reliability of the modified models.  相似文献   

18.
A 17 vol% SiCp/Al–Mg–Si–Cu composite plate with a thickness of 3 mm was successfully friction stir welded(FSWed) at a very high welding speed of 2000 mm/min for the first time. Microstructural observation indicated that the coarsening of the precipitates was greatly inhibited in the heat-affected zone of the FSW joint at high welding speed, due to the significantly reduced peak temperature and duration at high temperature. Therefore, prominent enhancement of the hardness was achieved at the lowest hardness zone of the FSW joint at this high welding speed, which was similar to that of the nugget zone. Furthermore, the ultimate tensile strength of the joint was as high as 369 MPa, which was much higher than that obtained at low welding speed of 100 mm/min(298 MPa). This study provides an effective method to weld aluminum matrix composite with superior quality and high welding efficiency.  相似文献   

19.
吴玉梅  熊晓云  靳蓉  孙敬民  杨林  罗晓星 《金属学报》2005,10(10):1100-1103
目的: 观察本实验室合成的一种治疗阿尔茨海默氏症(AD)的药物(1-二甲基磷酰基-2, 2, 2 -三氯)-乙基-1-醇烟酸醋(NMF),对体外培养的皮层神经细胞活性的影响以及对海人藻酸(KA)所致的神经损伤的保护作用。方法: 采用体外培养皮层神经元的方法,解剖分离 15 d胚胎小鼠皮层神经细胞, 接种于 96孔板,48 h 后加药并培养 72 h,以 MIT 法 观察 NMF 对小鼠皮层神经细胞活性的影响;同时将接种于 24 孔板的细胞预先给予 NMF,d 3 时加或不加KA处理后,以台盼蓝染色鉴别并计数死、活细胞,可得出细胞的存活率。结果: NMF 明显促进胎鼠皮层神经元活性,其中 NMF1、0. 1、10nmol·L-1促进神经元活性增殖率分别高达 34.7%、37.4%、36. 7%, NMF 明显促进正常胎鼠皮层神经元存活卒,与对照组比较,10nmol·L-1 NMF 对皮层神经元的存活率分别提高 39.3%、73.5%。 NMF能显著 对抗 KA 所致的神经元损伤,与 KA 损伤组相比, NMF0.1、10、10nmol·L-1对损伤皮层神经元的保护率分别为 77.30%、80.10%、84.15%。结论: NMF 明 显促进胎鼠皮层神经元的洁性、提高正常皮层神经元,的存活卒,并能有效地保护KA所致的神经元损伤,提示 NMF 是一种很有潜力的治疗 AD 的药物。  相似文献   

20.
On the basis of energy and shape method for the determination of the valence bond (VB) structures of crystal, the valence bond structure of titanium is redetermined at room temperature and calculated in the whole temperature range of 0-1943K. The outer shell electronic distribution of Ti is e_c~(2.9907) · (s_c~(0.4980) d_c~(2.4927)) ef1.0093 in crystal. The temperature dependences of the VB structures of hcp and bcc phases are the same. The VB structures of hcp and bcc phases monotonically increase or decrease with the increase in temperature, but show discontinuous changes at the phase-transformation temperature 1155K.  相似文献   

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