高碳石煤流态化氧化焙烧提高钒的浸出率

采用流态化氧化焙烧方式预处理广西某难浸高碳石煤以提高钒的浸出率,对氧化焙烧过程的热力学和钒的氧化动力学进行了分析,并考察了流态化焙烧对钒浸出率的影响。结果表明:石煤在氧化焙烧过程中,碳、黄铁矿的氧化反应在热力学上比V(Ⅲ)氧化反应更易进行,它们的存在对钒氧化具有抑制作用。钒的氧化反应受扩散动力学控制,其表观活化能为347.00 kJ/mol。钒浸出率随焙烧温度的增加先增加后减小,当焙烧温度为700℃和750℃时,钒浸出率随焙烧时间的延长而增加;当焙烧温度为800℃,焙烧时间0.5 h时,钒浸出率最高,达97.51%,延长焙烧时间反而不利于钒浸出。与传统的钠化氧化焙烧法相比,浸出率高,环境污染少。     

熔融钒渣纯氧氧化钙化提钒(英文)

在实验室条件下对熔融态钒渣直接氧化钙化提钒新工艺进行研究。在反应过程中利用纯氧氧化,CaO作为添加剂,硫酸浸出熟料。采用XRD、XPS、SEM及EDS等手段对钒渣熟料进行分析,考察不同CaO/V2O5质量比与硫酸浓度对熟料中钒浸出的影响,并与现行焙烧工艺在能耗方面进行对比。结果表明:钒渣熟料中形成了钒的富集相,钒渣的氧化钙化产物主要为CaV2O5和Ca2V2O7,并对钒酸钙的形成机理进行了阐释;XRD和XPS分析得出熔渣中钒的氧化反应在供氧充足的情况下存在一定限制,CaO的增加能促进五价钒在熔渣中的稳定;在优化的实验条件下(CaO/V2O5质量比0.6,粒度120~150μm,浸出时间2 h,浸出温度90°C,液固比5:1 mL/g,H2SO4浓度20%,搅拌强度500 r/min),钒的浸出率能达到90%;能耗计算得到每处理1000 kg钒渣,利用新工艺可以节约能量1.85×106 kJ。实验与计算结果验证新工艺是一种节能减排的提钒手段。     

机械活化强化钒渣钙化提钒工艺

针对转炉钒渣钙化焙烧酸浸工艺中存在的钒转浸率低的问题,采用高能球磨对钒渣进行活化预处理,以期强化其提钒效果。采用激光粒度分析仪、BET比表面积测定仪和XRD对活化前后钒渣进行了粒度、比表面积及物相结构分析;采用浸出实验研究了机械活化对钙化焙烧和浸出的影响规律。结果表明:机械活化法增大了钒渣的比表面积,增加了晶格畸变与微观应力,使含钒物相充分解离,由此可改善钒渣钙化焙烧的动力学条件。在浸出20 min条件下,机械活化80 min可将钒浸出率提高10%,最佳焙烧温度降低100℃。     

含钒石煤的氧化焙烧机理

采用X射线衍射(XRD)、扫描电镜(SEM)和能谱分析(EDX)等技术对石煤氧化焙烧过程进行研究,考察焙烧对钒浸出的影响.结果表明:石煤在氧化焙烧过程中,有机质和黄铁矿首先被氧化,含钒伊利石晶体结构在750～850 ℃被破坏,V(Ⅲ)和V(Ⅳ)氧化反应达到平衡时,钒浸出率达到最大值;当焙烧温度高达1 050 ℃时,物料烧结使钒被包裹,这是在1 050 ℃焙烧后钒浸出率急剧降低的主要原因.     

KOH亚熔盐中钒渣的溶出行为

对钒渣在KOH亚熔盐体系中的分解动力学进行研究,考察反应温度、碱矿质量比、粒度、气流量等工艺参数对钒渣分解过程的影响,获得最优工艺参数,并对反应机理进行探讨。结果表明,反应温度是最重要的影响因素;钒渣最优浸出条件如下:在反应温度为180℃,碱矿比4:1,KOH碱浓度75%,搅拌速率700 r/min,反应时间300 min,常压通氧气流量为1 L/min的反应条件下,最终钒、铬的浸出率分别达到95%和90%以上。钒渣在KOH亚熔盐介质中氧化分解遵循缩核模型,并主要受内扩散控制,钒和铬分解的表观活化能分别为40.54和50.27 kJ/mol,钒铬尖晶石的氧化以铁橄榄石、石英相的氧化分解为前提。     

钒铬渣锰盐焙烧酸浸过程中钒、铬的分离行为EI北大核心CSCD

本文针对目前钒铬渣中钒铬组元难以实现高效环保分离的研究现状,以钒铬渣为研究对象,碳酸锰为焙烧添加剂,通过钒铬渣碳酸锰焙烧−酸浸工艺实现了钒铬的高效分离。通过正交试验设计研究碳酸锰加入量、焙烧温度、恒温时间和升温速率对钒铬浸出行为的影响。结果表明:焙烧过程中钒尖晶石与碳酸锰的分解产物Mn_(2)O_(3)结合生成酸溶性的焦钒酸锰Mn_(2)V_(2)O_(7),随后在浸出过程中进入液相。而铬与铁结合生成稳定的固溶体(Fe_(0.6)Cr_(0.4))_(2)O_(3),浸出后转移入渣相。当碳酸锰加入量(以n(MnO)/n(V_(2)O_(5))计)为2.0,焙烧温度为850℃,恒温时间为2 h,升温速率为5℃/min时,钒浸出率达到最大值89.37%,铬浸出率仅为0.10%,实现钒的高效提取与钒铬分离。     

钒渣钙化焙烧相变过程的机理分析

采用X射线衍射、扫描电镜及能谱分析对钒渣钙化焙烧相变机理进行研究。结果表明:钒渣主要物相为不规则多边形铁钒尖晶石和铁橄榄石,660℃时均已开始氧化分解,前者产物为固溶体R2O3和部分铁板钛矿微晶聚体及晶间少量钒酸锰,铁橄榄石740℃时已显著分解、结构破坏。随着温度的提高(660~900℃),氧化产物逐渐增多,微晶粒长大聚合,钒酸盐形态由少量浸染状逐渐向微质点、无定形熔态带状变化,并向渣粒外侧迁移。低于900℃时,钒酸盐中Mn含量较高,Ca含量偏低,实际生成的为钒酸锰盐;900℃以上时,Mn和Ca含量则逆向变化,形成焦钒酸钙;940℃时,渣粒出现液相,使部分焦钒酸钙与R2O3和玻璃相混杂,阻碍氧化反应。     

钒钛磁铁矿提钒尾渣浸取钒

采用硫酸氢氟酸次氯酸钠组合浸出体系浸取钒钛磁铁矿提钒尾渣中的钒,研究浸出过程中试剂浓度、浸出液固比、浸出温度、浸出时间、物料粒度对钒浸出率的影响。结果表明:钒的浸出率随试剂浓度、液固比、温度和时间的升高而增大;当矿物粒度小于0.20 mm时,钒浸出率有随矿物粒度变小而减小的趋势。在物料粒度0.15~0.25 mm、初始硫酸浓度150 g/L、初始氢氟酸浓度30 g/L、次氯酸钠加入量为矿量1.5%、矿浆液固比6:1、浸出温度90℃、浸出时间6 h、搅拌速度500 r/min的条件下,钒的浸出率可达85%以上。     

熔融钒渣析晶调控高效提钒机理

基于熔融钒渣在不同冷却制度下导致钠化焙烧-水浸工艺提钒率波动大的问题,本文采用光学显微镜(OM)、X射线衍射(XRD)、扫描电镜(SEM+EDS)及电子探针(EPMA)等表征方法,研究熔融钒渣中钒的析出及钒尖晶石结晶特征对钒提取率的影响,并深入探讨了析晶调控高效提钒机理。结果表明：熔融钒渣的水淬温度对熔融钒渣中钒的析出率、钒尖晶石结晶粒度及钒渣钠化焙烧-水浸过程钒物相转化率及浸出率影响显著。在熔融钒渣降温过程中,1400～900℃为尖晶石快速成核生长期,900℃水淬后,钒基本完成从液相向尖晶石固相中的迁移,结晶相以钒铁尖晶石为主,其中钒呈均匀分散状态;900℃后,尖晶石生长变缓,并以钛铁尖晶石沿钒尖晶石边缘析出为主,尖晶石内部仍呈现钒的“中心聚集效应”。对1400℃、900℃和400℃水淬钒渣(Water-quenched vanadium slag,WQVS)分别进行钠化焙烧-水浸试验,水淬钒渣粒度小于0.15 mm,m(Na₂CO₃)∶m(NaCl)∶m(WQVS)=10∶3∶100,焙烧温度为780℃,焙烧时间为200 min。将焙烧产...     

液相氧化法钒渣提钒研究及展望(英文)

针对从钒渣中提取钒、铬存在的问题,提出了一系列绿色液相氧化法,包括NaOH/KOH亚熔盐法和NaOH-NaNO3熔盐法。与传统钠化焙烧法工艺相比,新方法的操作温度由850°C降低至200~400°C,而钒、铬的提取率分别由75%和接近0提高至95%和90%,整个操作过程中无废气及毒渣排放。与焙烧法相比,新工艺在能耗、环境友好及矿物资源综合利用率方面显示出明显的优势,成为钒行业绿色化升级的有效替代方案。     

Effects of K2O-Li2O doping on surface and catalytic properties of Fe2O3/Cr2O3 system

The effects of K₂O and Li₂O-doping (0.5, 0.75 and 1.5 mol%) of Fe₂O₃/Cr₂O₃ system on its surface and the catalytic properties were investigated. Pure and differently doped solids were calcined in air at 400-600 °C. The formula of the un-doped calcined solid was 0.85Fe₂O₃:0.15Cr₂O₃. The techniques employed were TGA, DTA, XRD, N₂ adsorption at −196 °C and catalytic oxidation of CO oxidation by O₂ at 200-300 °C. The results revealed that DTA curves of pure mixed solids consisted of one endothermic peak and two exothermic peaks. Pure and doped mixed solids calcined at 400 °C are amorphous in nature and turned to α-Fe₂O₃ upon heating at 500 and 600 °C. K₂O and Li₂O doping conducted at 500 or 600 °C modified the degree of crystallinity and crystallite size of all phases present which consisted of a mixture of nanocrystalline α- and γ-Fe₂O₃ together with K₂FeO₄ and LiFe₅O₈ phases. However, the heavily Li₂O-doped sample consisted only of LiFe₅O₈ phase. The specific surface area of the system investigated decreased to an extent proportional to the amount of K₂O and Li₂O added. On the other hand, the catalytic activity was found to increase by increasing the amount of K₂O and Li₂O added. The maximum increase in the catalytic activity, expressed as the reaction rate constant (k) measured at 200 °C, attained 30.8% and 26.5% for K₂O and Li₂O doping, respectively. The doping process did not modify the activation energy of the catalyzed reaction but rather increased the concentration of the active sites without changing their energetic nature.     

Perpendicular magnetic anisotropy in 70 nm CoFe2O4 thin films fabricated on SiO2/Si(1 0 0) by the sol-gel method

Cobalt ferrite CoFe₂O₄ films were fabricated on SiO₂/Si(1 0 0) by the sol-gel method. Films crystallized at/above 600 °C are stoichiometric as expected. With increase of the annealing temperature from 600 °C to 750 °C, the columnar grain size of CoFe₂O₄ film increases from 13 nm to 50 nm, resulting in surface roughness increasing from 0.46 nm to 2.55 nm. Magnetic hysteresis loops in both in-plane and out-of-plane directions, at different annealing temperatures, indicate that the films annealed at 750 °C exhibit obvious perpendicular magnetic anisotropy. Simultaneously, with the annealing temperature increasing from 600 °C to 750 °C, the out of plane coercivity increases from 1 kOe to 2.4 kOe and the corresponding saturation magnetization increases from 200 emu/cm³ to 283 emu/cm³. In addition, all crystallized films exhibit cluster-like structured magnetic domains.     

Effect of air annealing on mechanical properties and structure of amorphous B4C films

Amorphous B₄C films were prepared by magnetron sputtering of the hot-pressed B₄C target in different regimes. Hardness, intrinsic stress and film structure were investigated in dependence on the annealing temperature in air.Changes in the film structure and composition were investigated by Raman spectroscopy, confocal microscopy, and electron probe microanalysis. It has been shown that an annealing at 500 °C for 1 h leads to stress reduction, slight thickness decrease and increase of film hardness. However already at 600 °C the film oxidation proceeds very intensively with formation of the phases of boron oxide and amorphous carbon in the surface layer. The thickness of the film decreases quickly.The film oxidation is accompanied by formation of numerous carbon hillocks and redistribution of film material after annealing in furnace at 500 and especially 600 °C. The oxidation of a-B₄C films as well as of the crystalline bulk samples starts in some locations and has clearly pronounced heterogeneous character that indicates heterogeneous structure of amorphous films as well as of bulk crystalline samples.Annealing in air for a long period shifts down the onset of formation of hillocks to 400 °C and changes in film morphology to 300 °C. Thus the upper temperature limit for application of a-B₄C films in air depends also on the exposure time at the operation temperature.     

Annealing temperature effect on the corrosion parameters of autocatalytically produced Ni-P and Ni-P-Al2O3 coatings in artificial seawater

Ni-P and Ni-P-Al₂O₃ amorphous alloy coatings with 9.3 and 8.3 wt.% P respectively were obtained by autocatalytic deposition at 90 °C on carbon steel substrates. The effect of annealing temperature (100, 200, 300, 400 and 500 °C) upon the corrosion parameters of the coatings in artificial seawater with pH 5.0 and 8.1 at room temperature was evaluated by potentiodynamic polarisation and electrochemical impedance spectroscopy. It was found that deposits annealed at 400 and 500 °C presented an increase of the charge transfer resistance and negligible changes on samples annealed at lower temperature. Polarisation tests showed a charge transfer controlled anodic kinetics on both Ni-P and Ni-P-Al₂O₃ deposits and diffusion controlled cathodic reaction in artificial seawater at pH 5.0 and 8.1. The coatings did not present passive behaviour in the electrolytes and impedance measurements showed a single time constant for all cases with the lowest double layer capacitance (C_dl) for samples annealed at 400 and 500 °C. The best corrosion parameters were observed on Ni-P and Ni-P-Al₂O₃ coatings annealed at temperatures higher than 400 °C, which is the temperature where crystallisation of this kind of coatings takes place.     

Epitaxial 0.65PbMg1/3Nb2/3O3-0.35PbTiO3 (PMN-PT) thin films grown on LaNiO3/CeO2/YSZ buffered Si substrates

Ferroelectric PMN-PT thin films with a thickness of 600 nm were epitaxially grown on buffered Si (0 0 1) substrates at a substrate temperature that ranged from 550 to 700 °C using pulsed laser deposition (PLD). LaNiO₃ (LNO) electrode thin films with a resistivity of ∼1900 μΩ cm were epitaxially grown on CeO₂/YSZ buffered Si (0 0 1) substrates. The PMN-PT thin films grown at 600 °C on LNO/CeO₂/YSZ/Si substrates had a pure perovskite and epitaxial structure. The PMN-PT films exhibited a high dielectric constant of about 1818 and a low dissipation factor of 0.04 at a frequency of 10 kHz. Polarization-electric-field (P-E) hysteresis characteristics, with a remnant polarization of 11.1 μC/cm² and a coercive field of 43 kV/cm, were obtained in the epitaxial PMN-PT films.     

Synthesis-structure relations for reactive magnetron sputtered V2O5 films

V₂O₅ films were grown onto MgO (100) substrates by reactive magnetron sputtering between 26 °C to 300 °C to establish a detailed synthesis-structure relation. The effect of deposition temperature on structural characteristics and surface morphology was characterized using X-ray diffraction, Raman spectroscopy, atomic force microscopy and scanning and transmission electron microscopy. Films prepared at room temperature are amorphous while those deposited above 80 °C exhibit a polycrystalline structure with the orthorhombic symmetry of the V₂O₅ phase.     

The high-temperature oxidation behavior of vanadium-aluminum alloys

The oxidation behavior in air of pure vanadium, V-30Al, V-30Al-10Cr, and V-30Al-10Ti (weight percent) was investigated over the temperature range of 700–1000° C. The oxidation of pure vanadium was characterized by linear kinetics due to the formation of liquid V₂O₅ which dripped from the sample. The oxidation behavior of the alloys was characterized by linear and parabolic kinetics which combined to give an overall time dependence of 0.6–0.8. An empirical relationship of the form: W/A=Bt + Ct^1/2 + D was found to fit the data well, with the linear contribution suspected to be from V₂O₅ formation for V-30Al and V-30Al-10Cr, and a semi-liquid mixture of V₂O₅ and Al₂O₃ for V-30Al-10Ti. The parabolic term is presumed related to the formation of a solid mixture of V₂O₅ and Al₂O₃ for V-30Al and V-30Al-10Cr, and TiO₂ for V-30Al-10TiThe addition of aluminum was found to reduce the oxidation rate of vanadium, but not to the extent predicted by the theory of competing oxide phases proposed by Wang, Gleeson, and Douglass. This was attributed to the formation of a liquid-oxide phase in the initial stages of exposure from which the alloys could not recover. Ternary additions of chromium and titanium were found to decrease the oxidation rate further, with chromium being the most effective. The oxide scales of the alloys were found to be highly porous at 900° C and 1000° C, due to the high vapor pressure of V₂O₅ above 800° C.     

The corrosion of Ni3Al in a combustion gas with and without Na2SO4-NaCl deposits at 600–800°C

The corrosion behavior of Ni₃Al containing small additions of Ti, Zr, and B in combustion gases both with and without Na₂SO₄–NaCl deposits at 600–800°C has been studied for times up to four days. The corrosion of the saltfree Ni₃Al leads to the formation of very thin alumina scales at 600°C but of mixed NiO–Al₂O₃ scales containing also some sulfur compounds at higher temperatures, while the rate increases with temperature up to 800°C. The presence of the salt deposits considerably accelerates the corrosion rate, especially at 600 and 800°C. The duplex scales formed at 600°C are composed mostly of a mixture of NiO and unreacted salt in the outer layer and of alumina and aluminum sulfide with some nickel compounds in the inner layer. The scales grown at 700°C contain only one layer of complex composition, while those grown at 800°C are similar but have an additional outer layer containing similar amounts of nickel and aluminum. At 600 and 700°C NiSO₄ can be detected also in the salt layer. The samples corroded at 700°C and 800°C also show an Al-depleted zone containing titanium sulfide precipitates at the surface of the alloy. The hot corrosion of Ni₃Al involves a combination of various mechanisms, including fluxing of the oxide scale as well as mixed oxidation-sulfidation attack. At all temperatures Ni₃Al shows poor resistance to hotcorrosion attack as a result of the formation of large amounts of Ni compounds in the scales.     

Li4SiO4 氚增殖陶瓷的制备及其与14Cr-ODS钢的腐蚀界面行为

Li₄SiO₄小球与ODS钢的化学相容性对聚变反应器的安全运行具有重要意义。研究了在500、600、700 ℃的氩气环境中保温300 h后ODS钢与小球接触界面组织和成分的变化。结果表明,在600~700 ℃时,Li₄SiO₄小球与ODS钢的界面发生了严重的元素互扩散和反应。在Li₄SiO₄小球表面,由于ODS钢中Fe和Cr的扩散,出现了一层薄薄的反应层,这也导致了密度的增加,破碎负荷从51 N （500 ℃）下降到32 N（700 ℃）。XRD图谱显示,ODS钢表面出现了LiCrO₂和LiFeO₂新相,说明Li₄SiO₄小球中的Li和O原子可以扩散到ODS中,与Fe、Cr元素在高温下发生反应形成腐蚀层。在700 ℃时,腐蚀层可分为2个氧化层。最外层是LiFeO₂和LiCrO₂的混合物,下一层主要是LiFeO₂。在ODS钢的表面,700 ℃/300 h条件下氧扩散系数为2.2×10^-14 cm²/s,这说明ODS钢作为一种包层结构材料,在未来的包层设计中需要一层耐腐蚀涂层。     

Synthesis and characterization of Y3Al5O12 and ZrO2-Y2O3 thermal barrier coatings by combustion spray pyrolysis

Y₃Al₅O₁₂ and ZrO₂-Y₂O₃ (8 mol% YSZ) coatings for potential application as thermal barrier coatings were prepared by combustion spray pyrolysis. Thermal cycling of as deposited coatings on stainless steel and FeCrAlY bond coat substrates was carried out at 1000 °C and 1200 °C to determine the thermal fatigue response. Structural and morphological studies on Y₃Al₅O₁₂ and 8 mol% YSZ coatings before and after thermal cycling have been carried out. It has been noted that the coatings on FeCrAlY substrates remain intact after 50 cycles between room temperature and 1200 °C, whereas the coatings on stainless steel show some minor damage such as peeling off near the periphery after 50 cycles at 1000 °C. Thermal diffusivity values of Y₃Al₅O₁₂ and 8 mol% YSZ films were measured by using photo thermal deflection spectroscopy and the values are lower than those of coatings produced by conventional techniques such as EBPVD and APS.