退火温度对Mm(NiCoMnAl)5/5%(质量分数)Mg2Ni储氢合金结构和电化学性能的影响

采用二步熔炼法制备了Mm(NiCoMnAl)5/5%(质量分数)Mg2Ni复合储氢合金,并对其在不同温度(1023、1123和1223K)下进行退火热处理10h。用X射线衍射(XRD)、扫描显微镜(SEM)和电化学测试方法研究了退火温度对合金结构和电化学性能的影响。结果表明,铸态Mm(NiCoMnAl)5/5%(质量分数)Mg2Ni复合合金由LaNi5相和少量的Mg2Ni相组成,而退火态合金由LaNi5相和(La,Mg)Ni3新相组成。合金的最大放电容量和高倍率放电性能随退火温度的升高呈现出先增强后减弱的变化规律,其中退火温度为1023K时,合金电极的上述性能均达到最佳。合金的容量保持率随退火温度的升高而单调地增大,60次充放电循环后容量保持率从铸态合金的86.6%增大到退火合金(1223K)的92.4%。     

退火对La0.75Mg0.25Ni3.5Cox（x=0，0.6）合金结构与电化学性能影响

为了改善La0.75Mg0.25Ni3.5Cox(x=0,0.6)合金电极的循环稳定性,对铸态合金在0.3MPa压力氩气保护下进行不同温度退火(1123、1223和1323K),保温时间均为10h.研究了退火温度对合金电化学性能的影响.X射线衍射(XRD)和扫描电镜(SEM)分析表明,铸态及1123K温度退火后合金主要由LaNi5、(La,Mg)2Ni7相及少量LaNi2相组成;退火温度为1223和1323K时,合金中LaNi2相消失,合金主要由LaNi5、(La,Mg)Ni3及(La,Mg)2Ni7相组成.电化学试验结果表明,随着退火温度增加,x=0及x=0.6的合金最大放电容量分别从铸态的343.7、319.2增加到1323K时的390.4、357.5mAh/g;同时退火改善合金的循环稳定性,100次充放电循环后,随着退火温度升高,x=0、0.6时合金的容量保持率(S100)分别从铸态的55.17%、58.22%增加到1323K时的76.66%、67.58%.     

退火温度对La0.8Mg0.2Ni3.3Co0.2Six（x=0、0.1）合金电化学贮氢性能的影响

采用真空感应熔炼制备了La0.8Mg0.2Ni3.3Co0.2Si x(x=0、0.1)电极合金,并将铸态合金进行真空退火处理,退火温度为900、950、1000和1050℃,保温时间为8h。用XRD分析了铸态及退火态合金的相结构,测试了铸态及退火态合金的电化学贮氢性能。结果表明,铸态及退火态合金均具有多相结构,包括两个主相(La,Mg)2Ni7和LaNi5以及一个残余相LaNi3。退火处理未改变合金的相组成,但使两个主相的含量发生明显改变。合金主相的晶格常数及晶胞体积随退火温度的增加而增加。铸态及退火态合金均具有良好的活化性能,第1次循环即可达到最大放电容量。退火处理明显改善了合金的电化学循环稳定性,合金的放电容量随退火温度的升高先增加后减小。合金的高倍率放电性能(HRD)、电化学交流阻抗谱(EIS)以及氢扩散系数(D)的测试表明,合金的电化学动力学随退火温度的升高先上升后降低。     

快淬对MlNi3.55Co0.75Mn0.4Al0.3/5wt% Mg2Ni复合储氢合金电化学性能的影响

为了改善AB5型储氢合金的放电容量和循环稳定性,研究了快淬速度对MlNi3.55Co0.75Mn0.4Al0.3/5wt%Mg2Ni复合储氢合金结构和电化学性能的影响.电感耦合等离子发射光谱(ICP)、X射线衍射(XRD)、扫描电镜(SEM/EDS)和透射电子显微镜(TEM)分析表明,铸态复合合金由LaNi5相和少量的Mg2Ni相组成,而快淬态复合合金却由(La,Mg)Ni3新相和LaNi5相组成.当快淬速度≥15 m/s时,复合合金中形成明显的纳米晶组织并伴有部分非晶化倾向.电化学性能测试表明,快淬态复合合金的最大放电容量和容量保持率随快淬速度的增大呈现出先增大后减少的变化规律,其中快淬速度为20 m/s时合金电极的最大放电容量达最大值344 mAh/g,经100次充放电循环后该电极的容量保持率为93.9%.     

退火温度对La0.8Mg0.2Ni3.3Co0.2Six(x=0、0.1)合金电化学贮氢性能的影响

采 用 真 空 感 应 熔 炼 制 备 了La0.8Mg0.2Ni3.3Co0.2Six(x=0、0.1)电极合金,并将铸态合金进行真空退火处理,退火温度为900、950、1000和1050℃,保温时间为8h。用XRD分析了铸态及退火态合金的相结构,测试了铸态及退火态合金的电化学贮氢性能。结果表明,铸态及退火态合金均具有多相结构,包括两个主相(La,Mg)2Ni7和LaNi5以及一个残余相LaNi3。退火处理未改变合金的相组成,但使两个主相的含量发生明显改变。合金主相的晶格常数及晶胞体积随退火温度的增加而增加。铸态及退火态合金均具有良好的活化性能,第1次循环即可达到最大放电容量。退火处理明显改善了合金的电化学循环稳定性,合金的放电容量随退火温度的升高先增加后减小。合金的高倍率放电性能(HRD)、电化学交流阻抗谱(EIS)以及氢扩散系数(D)的测试表明,合金的电化学动力学随退火温度的升高先上升后降低。     

La2-xMgxNi7.0(x=0.4,0.5,0.6,0.7,0.8)贮氢合金结构和电化学性能的研究

用高频感应熔炼的方法制备了La2-xMgxNi7.0(x=0.4,0.5,0.6,0.7,0.8)贮氢电极合金,采用x-ray衍射和XRD粉末衍射全谱拟合分析方法及电化学方法系统研究了随Mg含量的增加,该类合金相结构和电化学性能的变化规律,以及合金在不同退火温度(1123K,1203K,1253K)和不同退火时间(24h,72h,144h)下相结构和微观组织及电化学性能的变化规律.实验结果表明,该类合金由(La,Mg)2Ni7相(Ce2Ni7型结构)、LaNi5(CaCu5型结构)相、(La,Mg)Ni3相(PuNi3型结构)及少量未知相组成.随Mg含量的增加,电极电化学放电容量呈先升高后降低趋势,当x=0.6时达到最大值389.87mAh/g;当Mg含量进一步增加时,电化学放电容量迅速降低,x=0.8时电化学放电容量为188.34mAh/g;随Mg含量的增加,合金组织中(La,Mg)Ni3相和LaNi5相增多.退火处理很大程度上消除了LaNi5相,高温退火有利于(La,Mg)2Ni7相的生成,低温退火有利于(La,Mg)Ni3相生成.退火时间的延长对合金相结构影响不明显,但提高了合金组织均匀性,同时使电化学放电容量降低.不同的退火温度和退火时间对未知相影响不明显.本文研究表明,退火温度对(La,Mg)2Ni7合金相结构有重要影响,Mg含量是影响合金相结构和电化学放电容量的关键.     

相组成对La0.75 Mg0.25 Ni3.5储氢合金电化学性能的影响

La-Mg-Ni基超晶格储氢合金与传统AB5型合金相比,具有优越的电化学容量,近年来受到研究者们的广泛关注,但是其合金相组成复杂,综合电化学性能尤其是循环稳定性有待提高.本工作通过将A2B7型La0.75Mg0.25Ni3.5合金在1203 K下退火40 h,制备了只含有(La,Mg)2Ni7和(La,Mg)5Ni19超晶格结构的合金,并研究了相转变对合金电化学性能的影响.研究表明,铸态合金含有(La,Mg)Ni3、(La,Mg)2Ni7和(La,Mg)5 Ni9超晶格相以及LaNi5相,在退火过程中,位于相图相对边缘位置的LaNi5相和(La,Mg)Ni3相消失,得到了只含有(La,Mg)2 Ni7和(La,Mg)5 Ni9超晶格的双相合金.超晶格相总量的增加伴随着元素组成的均匀化和应力的降低,这不但有效提高了合金的储氢容量,而且减轻合金在充/放电循环过程中的粉化和氧化,显著提高合金电极的循环稳定性.合金电极的最大放电容量由铸态的355 mAh·g-1提高到退火态的367 mAh·g-1,100周的循环稳定性由57.97％显著提高到81.47％.但是由于合金中的缺陷和晶界的减少,合金的高倍率放电性能有所降低.     

铸态和退火态A2B7型La-Mg-Ni系合金的电化学研究（英文）

为了改善铸态La3MgN i14合金的电化学性能,在0.3 MPa氩气气氛下对La3MgN i14合金进行了10 h退火处理,退火温度分别为1 123,1 223和1 323 K。采用X射线衍射(XRD)、扫描电镜(SEM)和电化学实验研究了合金的微观结构和电化学性能。结果表明,铸态及1 123 K温度退火后的合金由LaN i5相、(La,Mg)2N i7相以及少量的LaN i2相组成。1 223 K温度退火后合金含有LaN i5,(La,Mg)2N i7和(La,Mg)N i3相。1 323 K温度退火后合金的主相为LaN i5和(La,Mg)N i3相。与铸态合金相比,退火后合金组织更加均匀,晶粒长大。随着退火温度的增加,合金的一些电化学性能(如最大放电容量、放电效率、循环稳定性)以及动力学参数(如高倍率放电性能)增强,而电位差和电荷迁移电阻降低。在本研究范围内,为了放电容量和循环稳定性之间的平衡,铸态La3MgN i14合金的适宜退火温度为1 323 K。     

添加Si对La-Mg-Ni系A2B7型电极合金循环稳定性的影响

为了改善La-Mg-Ni系A2B7型电极合金的电化学循环稳定性,在合金中添加少量Si。采用真空感应熔炼制备了La0.8Mg0.2Ni3.3Co0.2Si x(x=0~0.2)电极合金,并将部分合金在真空条件下,温度为900、950、1000和1050℃下进行了退火处理。用XRD、SEM分析了铸态及退火态合金的微观结构,测试了铸态及快淬态合金的电化学循环稳定性。结果表明,铸态及快淬态合金均具有多相结构,包括两个主相(La,Mg)2Ni7和LaNi5及一个残余相LaNi3。添加Si使LaNi5相增加而(La,Mg)2Ni7相减少。合金的电化学循环稳定性随Si含量的增加而增加,当Si含量x从0增加到0.2时,铸态合金100次充放循环后的容量保持率(S100)从64.2%增加到73.1%,而950℃退火态合金的S100值从80.3%增加到93.7%。     

烧结工艺对贮氢合金La0.67Mg0.33Ni2.5Co0.5的微观组织结构及电化学性能影响的研究

系统研究了固相反应烧结方法制备La0.67Mg0.33Ni2.5Co0.5贮氢合金的烧结工艺对该合金的微观组织结构及电化学性能的影响规律.分析和研究了合金的微观组织结构、电化学放电性能及Mg含量的挥发损失问题.XRD和SEM及EPMA分析结果表明,在不同烧结条件下合金均由不合Mg的LaNi5相、富Mg的LaNi3相及一个贫Mg的LaNix(x=3.0～3.8)相三相组成.当烧结温度不超过1203k时合金主相为LaNi3相,当烧结温度超过1203K,LaNi5相逐步成为主相.原子吸收光谱分析结果表明,烧结温度不超过1203K,Mg元素没有明显损失;当烧结温度超过1203K,会引起Mg的大量挥发损失.电化学性能分析结果表明,烧结温度不超过1203K,合金放电能力主要受合金组织形成与均匀性影响;而烧结温度超过1203K,Mg元素挥发损失成为影响合金放电能力的决定因素.烧结条件为873～1123k保持24h、1203k保持2h,是制备La0.67Mg0.33Ni2 5Co0.5贮氢合金的适宜工艺.用该工艺制备的La0 67Mg0.33Ni2.5Co0.5贮氢合金Mg含量稳定(2.92%质量分数)、微观组织均匀、放电容量高(395mAh/g)、活化性能好(2个循环).     

Fe86Zr5.5 Nb5.5 B3非晶合金的超高压烧结成型

为了获得致密的块状Fe86Zr55Nb55B3纳米晶合金,研究了高压快速烧结工艺参数对样品致密度和α-Fe相晶粒尺寸的影响.结果表明:快淬球磨破碎非晶粉末在5.5 GPa/3min烧结条件下,当Pw=1150 W后,可获得相对密度为98.3%、单相α-Fe纳米晶(16.3 nm)块体合金,且随着Pw和t的增加,样品相对密度和α-Fe相晶粒尺寸均略有增加,样品典型的比饱和磁化强度σs和矫顽力Hc分别为119.6 emu/g,63.8 Oe.     

Thermodynamic properties of Pt5La,Pt5Ce,Pt5Pr,Pt5Tb and Pt5 Tm intermetallics

The Gibbs’ energies of formation of Pt₅La, Pt₅Ce, Pt₅Pr, Pt₅Tb and Pt₅ Tm intermetallic compounds have been determined in the temperature range 870–1100 K using the solid state cell: $$Ta,M + MF_3 /CaF_2 /Pt_5 M + Pt + MF_3 ,Ta$$ . The reversible emf of the cell is directly related to the Gibbs’ energy of formation of the Pt₅M compound. The results can be summarized by the equations: $$\begin{gathered} \Delta G_f^ \circ \left\langle {Pt_5 La} \right\rangle = - 373,150 + 6 \cdot 60 T\left( { \pm 300} \right)J mol^{ - 1} \hfill \\ \Delta G_f^ \circ \left\langle {Pt_5 Ce} \right\rangle = - 367,070 + 5 \cdot 79 T\left( { \pm 300} \right)J mol^{ - 1} \hfill \\ \Delta G_f^ \circ \left\langle {Pt_5 Pr} \right\rangle = - 370,540 + 4 \cdot 69 T\left( { \pm 300} \right)J mol^{ - 1} \hfill \\ \Delta G_f^ \circ \left\langle {Pt_5 Tb} \right\rangle = - 372,280 + 4 \cdot 11 T\left( { \pm 300} \right)J mol^{ - 1} \hfill \\ \Delta G_f^ \circ \left\langle {Pt_5 Tm} \right\rangle = - 368,230 + 4 \cdot 89 T\left( { \pm 300} \right)J mol^{ - 1} \hfill \\ \end{gathered} $$ relative to the low temperature allotropic form of the lanthanide element and solid platinum as standard states The enthalpies of formation of all the Pt₅M intermetallic compounds obtained in this study are in good agreement with Miedema’s model. The experimental values are more negative than those calculated using the model. The variation of the thermodynamic properties of Pt₅M compounds with atomic number of the lanthanide element is discussed in relation to valence state and molar volume.     

Synthesis of tritium-labeled 5-fluorouracil and 5-fluorocytosine

The effect of various catalysts and temperature on the solid-phase isotope exchange of 5-fluorouracil and 5-fluorocytosine with tritium was studied. The isotope exchange yielding the desired compounds is accompanied by dehalogenation and hydrogenation of the 5,6-double bond of the pyrimidine ring. Performing the reaction at a temperature below 160°C allowed the process to be carried out selectively, i.e., with the preservation of the functional groups and double bond in the starting compound. The yields of various products formed in the reactions of tritium with the above compounds were estimated. Synthesis conditions were found, and tritium-labeled 5-fluorouracil and 5-fluorocytosine were prepared with the molar radioactivity of 0.45 Ci mmol⁻¹ (16.7 TBq mol⁻¹) and 4.4 Ci mmol⁻¹ (0.16 PBq mol⁻¹), respectively, and with the purity exceeding 98%.     

Characterization of coprecipitated ferroelectric Bi2 VO5·5

Fine powders of orthorhombic bismuth vanadate (Bi₂ VO_5·5) have been synthesized by coprecipitation method. Powder X-ray diffraction and electron microscopic techniques have been used to characterize these samples. The formation of the monophasic Bi₂ VO_5·5 was confirmed. The compacted powders sintered at 1070K have been characterized for their dielectric properties as a function of both temperature (300–900 K) and frequency (100 Hz–10 MHz) and found to be superior to those obtained by the conventional solid-state reaction route.     

Evolution of the structure of Ti-5Al-5Mo-5V alloy deformed by high pressure

Specific features of straining of the Ti-5Al-5Mo-5V (VT22) alloy deformed by high pressure (cold and hot screw extrusion) are studied depending on its phase composition by the methods of X-ray diffraction analysis, optical microscopy, and electron microscopy. It is shown that the application of high pressure and complex schemes of deformation in combination with the action of temperature enables one to attain high levels of strains in the material without fracture. Under these conditions, new structures (containing nanosized particles responsible for the new properties) are formed. The mechanisms of deformation on the mesolevel are specified. It is shown that, in the process of cold hydroextrusion, the alloy in the one-phase β-state is deformed according to the mechanism of rotation via the formation of strain-induced martensite, whereas the alloy in the two-phase state is deformed according to the mechanism of bending. It is also shown that the mechanisms of deformation strongly depend on the initial phase composition of the alloy. The procedure of hot screw extrusion is characterized by the action of several mechanisms of deformation. Knowing these mechanisms, it is possible to choose the required modes of treatment and obtain structures guaranteeing the optimal combination of strength and plasticity. __________ Translated From Fizyko-Khimichna Mekhanika Materialiv, Vol. 42, No. 3, Pp. 57–64, May–June, 2006.     

DFT方法对LaNi5及LaNi5H0.5晶体结构的预测

根据密度泛函理论,以扩展平面波函数为基集,采用超软赝势技术,对LaNi5 储氢合金及其吸氢后的晶胞模型进行了优化,从理论上给出了其结构参数及性质。计算结果表明该方法能较好地符合 LaNi5 及其氢化物结构的实验值,为该类合金的结构预测提供了一个理论估算途径。此外,根据模型的结构参数分析了LaNi5 中不同间隙位的吸氢稳定性,解释了影响间隙位稳定性的因素。     

GAMS5

The construction of the double-crystal γ-spectrometer GAMS5 was finished recently and the instrument is now operational. Measurements with double flat crystals were carried out and we will report here on the progress concerning the characteristics of the spectrometer.     

Study of the hot deformation behaviour in Ti-5Al-5Mo-5V-3Cr-1Zr

Structural applications of near beta titanium alloys are gradually increasing in the aerospace industry because of their high specific mechanical properties and good corrosion resistance. Furthermore, a wide range of microstructures can be obtained by thermomechanical processes. This work determines by the use of EBSD technique the mechanism of restoration active in the near beta titanium alloy Ti-5Al-5Mo-5V-3Cr-1Zr for deformations in both α + β and β field near to the β transus temperature (T_β = 803 °C). Hot compression tests are carried out up to 0.7 true strain by means of a Gleeble^® 1500 machine at strain rates of 0.01, 0.1 and 1 s⁻¹. Dynamic recovery of β phase and rotation of the α grains take place predominantly in the α + β field. Further deformation produces continuous dynamic recrystallization of the β phase influenced by the strain rate. Dynamic recovery is observed during deformation above the T_β, where the misorientation is increasing towards the grain boundaries forming new small grains with a substructure at high strain rates and larger deformation. The stress exponent and the apparent activation energy for the sinh constitutive equations are determined and the microstructural features are correlated with the Zener-Hollomon parameter.