Bi3.25La0.75Ti3O12纳米管的制备工艺研究

研究了一种Bi3.25La0.75Ti3O12 (BLT)铁电存储材料纳米管的简单有效合成方法。通过阳极氧化铝模板(AAO)辅助溶胶凝胶法,合成了BLT纳米管。其基本过程是以次硝酸铋、硝酸镧和钛酸四丁酯为原料,以冰醋酸和乙二醇甲醚为溶剂配制BLT溶胶,然后将BLT溶胶滴在AAO模板表面,浸润后烘干并反复多次,而后将材料在500 ℃下保温1 h,除去有机物,最后在750 ℃下保温30 min晶化,用KOH腐蚀去除氧化铝模板,即得到BLT纳米管。结果表明,BLT纳米管具有[117]择优取向;BLT纳米管管壁光滑,直径与模板孔径相当,约300 nm,且分布均匀,管壁厚度约25 nm,纳米管是多晶体,由粒径为8~12 nm晶粒组成     

Bi_(3.15)Nd_(0.85)Ti_3O_(12)纳米管阵列的制备与微结构表征

采用溶胶凝胶法,在孔径为200 nm的阳极氧化铝模板中制备了Bi_3.15Nd_0.85Ti_3O_(12)纳米管阵列.通过XRD、SEM、TEM、HRTEM、SAED和Raman光谱测试手段对纳米管阵列的物相、微结构和声子振动特性进行了表征.研究表明,所合成BNdT纳米管为钙钛矿相多晶结构,纳米管外径约为200 nm,管壁厚约10 nm,管径和长度与所用AAO模板尺寸一致.Raman光谱分析表明,Nd离子取代了类钙钛矿层中A位的Bi离子.     

溶胶凝胶模板法合成ITO纳米管及其氢敏性能

采用简单的溶胶凝胶阳极氧化铝模板法制备了ITO纳米管.通过FE-SEM、HRTEM、XRD对其微观形貌、结构、相组成等进行了表征和分析,并测试了其对H_2的气敏特性.结果表明,所得纳米管是由10～20 nm晶粒组成的多晶结构,壁厚约为25 nm,平均直径约250 nm,与AAO (Anodic Aluminum Oxide)模板的直径相同.产物在550 ℃热处理后为立方铁锰矿结构的In_2O_3,Sn~(4+)已经掺杂到In_2O_3的晶格中.所得ITO纳米管常温下对氢气具有较好的敏感性及稳定性.     

原位模板法在铝基底上制备TiO2纳米管阵列薄膜

采用液相沉积法，将铝基多孔阳极氧化铝（AAO）模板浸入到（NH4）2TiF6溶液中，制备出高度有序的TiO2纳米管阵列薄膜，并在不同的温度下进行了热处理。用场发射扫描电子显微镜、透射电子显微镜和X射线衍射仪等手段对试样的微观形貌、结构及物相进行了表征。结果表明，TiO2纳米管的形貌依赖于AAO的特征，薄膜是由外径大约200nm，壁厚约40nm的TiO2纳米管阵列组成，薄膜厚度约25μm。原位模板法制备的TiO2纳米管阵列薄膜为非晶态，在400℃空气中焙烧2h转变为锐钛矿相TiO2。经过650℃焙烧仍保持纳米管结构，表现出较好的热稳定性。     

溶胶一凝胶模板法制备氧化镍纳米线

采用二次阳极氧化的方法,以5%磷酸为电解液,制得具有一定厚度有序性较高的阳极氧化铝模板(AAO),结合溶胶-凝胶法在模板微孔内合成氧化镍纳米线.利用扫描电镜(SEM)对模板和纳米线材料的形貌进行了表征,结果表明:采用该方法成功制得线状的氧化镍,长度可达亚微米级,直径约为100nm,与AAO模板的孔径大小基本一致,因此可以通过调节AAO模板的孔径大小来实现氧化镍纳米线的可控生长.     

Fe磁性纳米线阵列的制备与微波吸收性能研究

采用脉冲和直流电沉积方式，以FeSO4，（NH4）2SO4等混合溶液为电解液，在多孔阳极氧化铝模板（AAO模板）微孔内成功制备出Fe磁性纳米线阵列。用X射线衍射仪、扫描电镜及HP8510B网络分析仪对多孔AAO模板以及Fe磁性纳米线阵列的微观形貌、组织结构及微波吸收性能进行了测试。结果表明，沉积的纳米线为立方结构α=Fe，且纳米线阵列存在（110）择优取向性。Fe纳米线组装后的铝基AAO模板吸波材料具有良好的微波吸收效果，在2GHz～18GHz频段内的最大反射率为-4．8dB，大于-1dB的吸收带宽约为10GHz。     

化学沉积法制备铜纳米管与纳米线

以多孔氧化铝膜为模板，通过化学沉积法制备Cu纳米管与纳米线。分别用透射电子显微镜（TEM）、X射线衍射仪（XRD）对制备的样品进行了形貌分析与结构表征。结果表明，成功组装出Cu纳米管与纳米线。研究发现，Cu纳米管与纳米线制备成功与否取决于前处理过程中的还原步骤。Cu纳米管的外径与Cu纳米线的直径可通过改变模板制备工艺，进而改变模板孔径来调节；Cu纳米管的内径可由沉积时间的变化来控制。     

PZT纳米晶粉体的水热合成及表征

本文选取近于MPB的组成Pb(Zr0.52Ti0.48)O3进行了研究.通过水热法合成了纯相钙钛矿型纳米晶锆钛酸铅(PZT)粉体.所用原料试剂为分析纯Pb(NO3)2、Zr(NO3)4·5H2O、Ti(OC4H9)4,NaOH作为矿化剂.原料试剂按Pb(Zr0.52Ti0.48)O3化学计量比混合放入50 mL内衬聚四氟乙烯的高压釜中,填充度为70%.高压釜在170～270℃之间选择一定温度加热2 h后在冰水中冷却到室温.前躯体及水热处理的粉体通过XRD和SEM进行表征.PZT相在220℃加热2 h开始出现.在270℃加热2 h合成了纯相钙钛矿型纳米晶PZT粉体.粉体的平均尺寸为25 nm.     

0-3型改性PZT／IPN压电复合材料的制备和性能研究

以溶胶-凝胶法制备改性PZT纳米陶瓷粉体，粉体直径50nm左右。以改性PZT陶瓷粉体为压电相，以同步法制备的互穿聚合物网络（IPN）为基体相，采用溶液混合法制备0-3型改性PZT／IPN复合材料。采用自制极化装置对复合体系进行电晕极化，极化电压为9．5kV、极化温度为100℃、极化时间为45min。对不同改性PZT含量的复合材料介电、压电性能检测结果表明：复合材料介电性能和压电性能介于有机和无机体系之间。随着PZT陶瓷含量的增加，复合材料的电性能参数逐渐接近陶瓷相。     

SiO2空心球闭孔减反膜的制备及性能研究

目的 在获得光伏/光热用SiO2减反膜高透过率的同时,提高其抗划伤性能和耐候性。方法 以聚丙烯酸（PAA, Mw~3000）为模板制备具有核壳结构的SiO2,离心水洗去除PAA模板,形成SiO2空心球,接着将空心球分散于无水乙醇中形成溶胶,然后将该溶胶与酸催化溶胶混合,形成复合溶胶,最后经浸渍提拉成膜、烧结后,在载玻片上制得SiO2空心球闭孔减反膜。用透射电子显微镜（TEM）和扫描电子显微镜（SEM）分别表征了空心球的微观结构和减反膜的表面形貌,利用紫外-可见分光光度计测试了减反膜的透过率,采用铅笔硬度测试和耐湿热测试（HAST）试验,分别检测了减反膜的抗划伤性能和耐候性。结果 TEM测试结果显示,制备的SiO2空心球结构完整,壁厚均匀。SEM图显示减反膜表面平坦。当SiO2空心球溶胶与酸催化溶胶的用量比例为9∶1时,减反膜透过率的峰值为98.1%,抗划伤硬度为5 H,经HAST试验后,其透过率为初始值的98.1%。结论 用离心水洗法去除PAA模板制备的空心球比烧结去除模板法的空心占比高,与酸催化溶胶混合后制得的SiO2空心球减反膜空隙率高、折射率低,从而其透过率得到提高。同时,减反膜闭孔结构使其表面致密平整,比开孔结构减反膜具有更高的抗划伤性能和耐候性,在户外太阳能光伏/光热玻璃表面减反方面具有重要的应用价值。     

Effects of Post-weld Heat Treatment on Microstructure,Mechanical Properties and the Role of Weld Reinforcement in 2219 Aluminum Alloy TIG-Welded Joints

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.     

The First Phase of the SRIF Industrialized Base in ＂West Area＂ Has Been Put into Operation

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.     

新型的治疗阿尔茨海默氏症药物(1-二甲基磷酰基-2,2,2-三氯)-乙基-1-醇烟酸醋对体外神经细胞的作用

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。     

THERMODYNAMICS STUDY ON THE DECOMPOSITION OF CHROMITE WITH KOH

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.     

INFLUENCE OF HEAT TREATMENT ON DAMPING BEHAVIOUR OF THE MAGNESIUM WROUGHT ALLOY AZ61

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.     

Three-Dimensional Growth of Coherent Ferrite in Austenite: A Molecular Dynamics Study

Coherent second phase often exhibits anisotropic morphology with specifi c orientations with respect to both the second and the matrix phases. As a key feature of microstructure, the morphology of the coherent particles is essential for understanding the second-phase strengthening eff ect in various industrial alloys. This letter reports anisotropic growth of coherent ferrite from austenite matrix in pure iron based on molecular dynamics simulation. We found that the ferrite grain tends to grow into an elongated plate-like shape, independent of its initial confi guration. The fi nal shape of the ferrite is closely related to the misfi t between the two phases, with the longest direction and the broad facet of the plate being, respectively, consistent with the best matching direction and the best matching plane calculated via the Burgers vector content(BVC) method. The strain energy calculation in the framework of Eshelby's inclusion theory verifi es that the simulated orientation of the coherent ferrite is energetically favorable. It is anticipated that the BVC method will be applicable in analysis of anisotropic growth and morphology of coherent second phase in other phase transformation systems.     

Effect of Rare Earth Doping on Impedance,Modulus and Conductivity Properties of Multiferroic Composites:0.5(BiLa_xFe_(1-x)O_3)–0.5(PbTiO_3)

The Lanthanum-doped bismuth ferrite–lead titanate compositions of 0.5(Bi LaxFe1-xO3)–0.5(Pb Ti O3)(x = 0.05,0.10,0.15,0.20)(BLxF1-x-PT) were prepared by mixed oxide method.Structural characterization was performed by X-ray diffraction and shows a tetragonal structure at room temperature.The lattice parameter c/a ratio decreases with increasing of La(x = 0.05–0.20) concentration of the composites.The effect of charge carrier/ion hopping mechanism,conductivity,relaxation process and impedance parameters was studied using an impedance analyzer in a wide frequency range(102–106Hz) at different temperatures.The nature of Nyquist plot confirms the presence of bulk effects only,and non-Debye type of relaxation processes occurs in the composites.The electrical modulus exhibits an important role of the hopping mechanism in the electrical transport process of the materials.The ac conductivity and dc conductivity of the materials were studied,and the activation energy found to be 0.81,0.77,0.76 and 0.74 e V for all compositions of x = 0.05–0.20 at different temperatures(200–300 °C).     

Using Finite Element and Contour Method to Evaluate Residual Stress in Thick Ti-6Al-4V Alloy Welded by Electron Beam Welding

This work was to reveal the residual stress profile in electron beam welded Ti-6Al-4V alloy plates(50 mm thick) by using finite element and contour measurement methods.A three-dimensional finite element model of 50-mmthick titanium component was proposed,in which a column–cone combined heat source model was used to simulate the temperature field and a thermo-elastic–plastic model to analyze residual stress in a weld joint based on ABAQUS software.Considering the uncertainty of welding simulation,the computation was calibrated by experimental data of contour measurement method.Both test and simulated results show that residual stresses on the surface and inside the weld zone are significantly different and present a narrow and large gradient feature in the weld joint.The peak tensile stress exceeds the yield strength of base materials inside weld,which are distinctly different from residual stress of the thin Ti-6Al-4V alloy plates presented in references before.     

Microstructures and Tensile Properties of Ultrafine-Grained Ni–(1–3.5) wt% SiC_(NP) Composites Prepared by a Powder Metallurgy Route

Silicon carbide nanoparticle-reinforced nickel-based composites(Ni–Si CNP),with a Si CNPcontent ranged from1 to 3.5 wt%,were prepared using mechanical alloying and spark plasma sintering.In addition,unreinforced pure nickel samples were also prepared for comparative purposes.To characterize the microstructural properties of both the unreinforced pure nickel and the Ni–Si CNPcomposites transmission electron microscopy(TEM) was used,while their mechanical behavior was investigated using the Vickers pyramid method for hardness measurements and a universal tensile testing machine for tensile tests.TEM results showed an array of dislocation lines decorated in the sintered pure nickel sample,whereas,for the Ni–Si CNPcomposites,the presence of nano-dispersed Si CNPand twinning crystals was observed.These homogeneously distributed Si CNPwere found located either within the matrix,between twins or on grain boundaries.For the Ni–Si CNPcomposites,coerced coarsening of the Si CNPassembly occurred with increasing Si CNPcontent.Furthermore,the grain sizes of the Ni–Si CNPcomposites were much finer than that of the unreinforced pure nickel,which was considered to be due to the composite ball milling process.In all cases,the Ni–Si CNPcomposites showed higher strengths and hardness values than the unreinforced pure nickel,likely due to a combination of dispersion strengthening(Orowan effects) and particle strengthening(Hall–Petch effects).For the Ni–Si CNPcomposites,the strength increased initially and then decreased as a function of Si CNPcontent,whereas their elongation percentages decreased linearly.Compared to all materials tested,the Ni–Si CNPcomposite containing 1.5% Si C was found more superior considering both their strength and plastic properties.     

Directional Growth of Tin Crystals Controlled by Combined Solute Concentration Gradient Field and Static Magnetic Field

A new method was introduced to achieve directional growth of Sn crystals. Microstructures in liquid(Pb)/liquid(Sn) diffusion couples were investigated under various static magnetic fields. Results show that the β-Sn crystals mainly reveal an irregular dendritic morphology without or with a relatively low static magnetic field(B0.3 T). When the magnetic field is increased to 0.5 T, the β-Sn dendrites close to the final stage of growth begin to show some directional character. With a further increase in the magnetic field to a higher level(0.8–5 T), the β-Sn dendrites have an enhanced directional growth character, but the dendrites show a certain deflection. As the magnetic field is increased to 12 T, the directional growth of the β-Sn dendrites in the center of the couple is severely destroyed. The mechanism of the directional growth of the β-Sn crystals and the deflection of the β-Sn crystals with the application of static magnetic field was tentatively discussed.