分散第二相Al_2O_3对高分子固体电解质电性能的影响

于固体电解质PEO＿NaSCN络合物中加入Al2O3绝缘体作为第二相,分别研究了Al2O3的粒径,含量对该固体电解质电性能的影响.发现当Al2O3的粒径小于1μm时,离子电导率比纯的固体电解质的电导率高,大于1μm时,则比纯样品的低,即临界粒径约为1μm.当Al2O3的含量达到约25%时,电导率达到极大值.此外,样品的高频极化和低频极化也随Al2O3的粒径的增大而越显著.     

LaF_3-LiF-La_2O_3系熔盐密度的研究

根据阿基米德定律,测定了La F3-Li F-La2O3熔盐电解质体系的密度,研究了温度、La F3的含量、La2O3加入量对体系密度的影响。结果表明:密度随着温度的升高呈明显线性降低的趋势,而随着La F3含量的增加而增大。在温度为1050℃时,La F3摩尔含量为20%~35%的该熔盐电解质体系的密度随着La2O3加入量的增加先增加后降低,在La2O3的饱和溶解度(1.5%~3%)附近达到最大值。     

新型电解质材料CaZr_(0.1)Ti_(0.9)O_3的制备与电性能

采用溶胶-燃烧法合成了可用于固体氧化物燃料电池(SOFC)的新型固体电解质材料CaZr_(0.1)Ti_(0.9)O_3.通过XRD、交流复阻抗等电化学方法对样品的结构、电导性能进行了表征,并考察了材料的烧结性能. 结果表明,溶胶-燃烧法可以成功制备出具有良好烧结性能的CaZr_(0.1)Ti_(0.9)O_3电解质粉末,1 400 ℃下得到的烧结体的相对密度可达到95%. 电性能测试表明,CaZr_(0.1)Ti_(0.9)O_3烧结体在中温范围内具有较高的氧离子电导率(σ_(800 ℃)＝2.24×10~(-3)S/cm)、低的电导活化能(0.89 eV).     

Ce_(0.8)Sm_(0.2)O_(1.9)固体电解质的电子电导性研究

应用溶胶-凝胶法制备了Ce_(0.8)Sm_(0.2)O_(1.9)固体电解质粉体,通过X射线衍射对所制备的电解质粉体进行了物相分析。研究表明,Sm2O3已经固溶到CeO_2中形成了具有萤石结构CeO_2基固溶体。经成型并在1450℃下烧结2 h获得致密的Ce_(0.8)Sm_(0.2)O_(1.9)固体电解质。通过组装含有氧离子阻塞电极电池(-)致密Al2O3,Pt|Ce_(0.8)Sm_(0.2)O_(1.9)(SDC)固态电解质|Pt,O2(+)测试空气中不同温度下的电子电导。应用扫描电子显微镜观察所制备试样的微观组织形貌,结果表明:制备的电解质组织致密,高温粘合剂、电解质及刚玉坩埚结合紧密,保证了阻塞电极的气密性。采用Hebb-Wagner离子阻塞电极法测定了Ce_(0.8)Sm_(0.2)O_(1.9)在空气气氛下的电子导电性。结果显示:在测量温度范围内Ce_(0.8)Sm_(0.2)O_(1.9)固体电解质的电子电导率在1×10-8~1×10-6m S·cm-1之间,经计算得出活化能的平均值为0.9885 e V。     

固体过氧钼酸的制备及其性质研究

本文提供了制备固体过氧钼酸的新方法,它以Na_2MoO_4为原料,按Mo:H_2O_2=2.00:1.05(摩尔比)和游离酸度为0.40mole/dm~3的量加入H_2O_2和HNO_3,然后在50℃条件下加热20小时,析出Mo:(O_2):H_2O=2:1:2的固体过氧钼酸,得率96%。用热分析和超高真空程序升温质谱研究了它的性质,并推断其可能结构。     

EDTA配合法制备beta-Al_2O_3固体电解质

以金属硝酸盐和乙二胺四乙酸(EDTA)为原料,采用EDTA配合溶胶-凝胶法制备了beta-Al2O3前驱粉料,并利用X射线衍射分析(XRD)、红外光谱分析(FTIR)、热分析(TG/DSC)、交流阻抗谱(EIS)和扫描电镜(SEM)等测试技术对beta-Al2O3的合成工艺进行了详细的研究。结果表明:该法合成beta-Al2O3前驱粉料的温度为1150℃,比固相反应法低了150℃,平均粒径约为42nm,具有较好的成型和烧结性能。将素坯在1630℃保温烧结,得到的烧结体相对密度为96%以上,300℃时beta-Al2O3固体电解质的离子电导率为0.026S·cm-1。     

共压直接成型法制备单腔体固体氧化物燃料电池

采用共压直接成型法制备单腔体固体氧化物燃料电池(SC-SOFC),单电池结构为Ni-YSZ/YSZ/LSM,YSZ为8%(x)Y2O3稳定的ZrO2,LSM为锰酸镧锶(La0.7Sr0.3MnO3).应用扫描电子显微镜(SEM)研究了电池微观结构,结果表明:阴极和电解质之间结合紧密,LSM在阴极YSZ三维骨架上负载性能良好;YSZ电解质薄膜厚约50μm,阳极厚约600μm,阴极层厚约100μm.研究了单电池反应温度T,阴极催化剂负载层数n,甲烷和氧气混合体积比Rmix对电池输出性能的影响规律.在T=800℃、n=2、Rmix=2时,电池性能达到最佳,开路电压为0.95V,最大电流密度为130mA·cm-2,最大功率密度为30mW·cm-2.     

离子液体协同固体超强酸催化花生壳制备乙酰丙酸

以离子液体氯化1-丁基-3-甲基咪唑鎓([Bmim]Cl)为溶剂,以6种S2O82-/MxOy型固体超强酸为催化剂,将微波预处理后的花生壳水解,制备乙酰丙酸。研究表明,S2O82-/Zr O2-Al2O3-Si O2固体酸的催化效果最佳,进一步考察了反应时间、反应温度、固体酸用量、水含量对乙酰丙酸产率的影响。由响应面法(RSM)建立的二次回归模型得到优化水解工艺条件,即:在固体酸用量为5.1(wt)%条件下于160℃反应51min,乙酰丙酸产率可达到78.3%。固体酸再生重复使用效果良好。     

Al含量对Pt-SO2-4/ZrO2-Al2O3固体超强酸催化正戊烷异构化性能的影响

通过向SO42-/ZrO2催化剂中同时引入适量的Pt和Al2O3,制备出了具有较高催化性能和稳定性的Pt-SO42-/ZrO2-Al2O3型固体超强酸催化剂.以正戊烷异构化反应为探针,考察了Al含量对催化剂性能的影响;并采用X射线衍射(XRD)、比表面积测定(BET)、红外(IR)光谱、程序升温还原(TPR)、热重-差热分析(TG-DTA)和氨-程序升温脱附(NH3-TPD)手段对催化剂进行了表征.结果表明,Al能够提高ZrO2的晶化温度,抑制硫的分解,增加催化剂的比表面积,增强硫氧键的结合,提高催化剂的还原性能,增加催化剂的酸强度和酸总量.当Al2O3含量(质量分数,w)为5.0%时,Pt-SO42-/ZrO2-Al2O3固体超强酸催化剂的催化活性最好,在100 h内异戊烷收率可稳定在52.0%以上,选择性在98.2%以上.     

离子液体协同固体酸催化花生壳制备乙酰丙酸的研究

以离子液体氯化1-丁基-3-甲基咪唑鎓([Bmim]Cl)为溶剂,以6种S2O82-/MxOy型固体超强酸为催化剂,将微波预处理后的花生壳水解,制备乙酰丙酸。研究表明,S2O82-/Zr O2-Al2O3-Si O2固体酸的催化效果最佳,进一步考察了反应时间、反应温度、固体酸用量、水含量对乙酰丙酸产率的影响。由响应面法(RSM)建立的二次回归模型得到优化水解工艺条件,即:在固体酸用量为5.1(wt)%条件下于160℃反应51min,乙酰丙酸产率可达到78.3%。固体酸再生重复使用效果良好。     

中温复合固体电解质SDC-LSGM的制备和性能

采用甘氨酸-硝酸盐法分别制备了Ce0.85Sm0.15O2-δ(SDC)与La0.9Sr0.1Ga0.8Mg0.2O3-δ(LSGM)两种电解质材料, 并用固相混合法将两种材料按不同质量比(SDC与LSGM的质量比分别为9∶1, 8∶2, 5∶5)混合制备复合电解质材料. 采用交流阻抗技术对样品的电学性能进行研究. 实验结果表明, SDC与LSGM的质量比为9∶1(SL91)时, 样品具有较高的电导率, 在350—800 ℃温度范围内其电导率均比SDC的高. 以复合电解质为支撑体, 以Sm0.5Sr0.5CoO3 为阴极、NiO/SDC 为阳极制成单电池, 测试结果显示, 在800 ℃时以SL91为电解质的单电池的最大输出功率密度为0.25 W/cm2, 最大电流密度为1.06 A/cm2. 在电池的工作温度区间(600—800 ℃)内以复合材料为电解质的单电池的开路电压比以SDC为电解质的高.     

Research of High Temperature Crystalline Structure and Property Evolution of Magnesium Aluminate Spinel

Magnesium aluminate spinel （MgAl2O4） with high purity has been prepared by using anodized waste slag from aluminum factory and （MgCO3）4Mg（OH）2.5H2O as the main raw materials to discuss the change laws and characteristics of crystalline structure, microstructures and properties. X-ray diffraction （XRD） and scanning electron microscopy （SEM）, together with relevant analysis software, were used to characterize the crystal phases and microstructures so as to get MgAl2O4. Results show that when increasing the holding time the amount of MgAl2O4 increases fwstly and then keeps stable, but bulk density and bending strength increase firstly and then decrease. The best holding time is determined to be 3 h because at this time the corresponding MgAl2O4 content is up to 93%, bulk density 3.23 g·cm^3, apparent porosity 4.6% and bending strength 122.4 MPa.     

镓酸镧基中温-SOFC的新型阳极NiO-La0.3Ce0.7O2-δ研究

采用共沉淀法制备了NiO-La0.3Ce0.7O2-δ(LDC30)新型阳极材料, 通过对其配方与性能的研究, 探索获得中温SOFC高性能阳极材料的新途径.     

YSZ传导膜H_2S固体氧化物燃料电池

研究了Y2O3稳定的ZrO2(YSZ)氧离子传导膜H2S固体氧化物燃料电池性能。掺杂NiS、电解质、Ag粉和淀粉制备了双金属复合MoS2阳极催化剂,掺杂电解质、Ag粉和淀粉制备了复合NiO阴极催化剂,用扫描电镜对YSZ和膜电极组装(MEA)进行了表征,比较了不同电极催化剂的性能和极化过程,考察了不同温度对电池性能的影响。结果表明,双金属复合MoS2/NiS阳极催化剂在H2S环境下比Pt和单金属MoS2催化剂稳定,复合NiO阴极催化剂比Pt性能好,在电极催化剂中加入Ag可显著提高电极的导电性;与Pt电极相比,复合MoS2阳极和复合NiO阴极催化剂的过电位较小,阳极的极化比阴极侧小;温度升高,电池的电流密度与功率密度增加,电化学性能变好。在750℃、800℃、850℃和900℃及101.13 kPa时,结构为H2S、(复合MoS2阳极催化剂)/YSZ氧离子传导膜/(复合NiO阴极催化剂)、空气的燃料电池最大功率密度分别为30 mW/cm2、70 mW/cm2、155 mW/cm2及295 mW/cm2、最大电流密度分别为120 mA/cm2、240 mA/cm2、560 mA/cm2和890 mA/cm2。     

基于氧化镍沉积硅胶固相萃取与液相色谱-质谱联用技术的2型糖尿病血清中咪唑丙酸的检测

咪唑丙酸可以通过哺乳动物雷帕霉素靶蛋白复合物1(mTORC1)路径引起人的胰岛素抵抗, 从而导致2型糖尿病(T2D), 因此, 咪唑丙酸的准确定量可辅助2型糖尿病的诊断. 本文利用NiO与咪唑基团之间的配位作用, 采用氧化镍沉积硅胶(NiO@SiO₂)萃取材料对咪唑丙酸进行选择性富集和萃取. 首先对NiO@SiO₂ 固相萃取(SPE)条件进行优化: 吸附剂用量为200 mg, 上样液为20 mmol/L的磷酸盐缓冲溶液(pH=3.0), 解吸液为1.0 mL含1%(质量分数)NH₃·H₂O的水溶液; 然后, 对萃取液进行高效液相色谱-质谱(HPLC-MS)分离分析, 建立了血清中咪唑丙酸的检测方法. 结果表明, 咪唑丙酸浓度在0.05~10 ng/mL范围内对质谱响应值具有良好的线性关系(R ²≥0.996), 检出限和定量限分别为0.02和0.05 ng/mL, 加标回收率为84.0%~119%, 相对标准偏差RSD<17.2%. 将该方法用于检测2型糖尿病患者与正常人血清样品中的咪唑丙酸, 发现在2型糖尿病患者与正常人的血清中咪唑丙酸含量存在显著性差异, 说明咪唑丙酸的准确定量对2型糖尿病具有医学诊断上的潜力.     

Monolayer dispersion of NiO in NiO/Al2O3 catalysts probed by positronium atom

NiO/Al(2)O(3) catalysts with different NiO loadings were prepared by impregnation method. The monolayer dispersion capacity of NiO is determined to be about 9 wt.% through XRD quantitative phase analysis. Positron lifetime spectra measured for NiO/Al(2)O(3) catalysts comprise two long and two short lifetime components, where the long lifetimes τ(3) and τ(4) correspond to ortho-positronium (o-Ps) annihilation in microvoids and large pores, respectively. With increasing loading of NiO from 0 to 9 wt.%, τ(4) drops drastically from 88 to 38 ns. However, when the NiO loading is higher than 9 wt.%, τ(4) shows a slower decrease. Variation of λ(4) (1/τ(4)) as a function of the NiO content can be well fitted by two straight lines with different slopes. The relative intensity of τ(4) also shows a fast decrease followed by a slow decrease for the NiO content lower and higher than 9 wt.%, respectively. The coincidence Doppler broadening measurements reveal a continuous increase of S parameter with increasing NiO loading up to 9 wt.% and then a decrease afterwards. This is due to the variation in intensity of the narrow component contributed by the annihilation of para-positronium (p-Ps). Our results show that the annihilation behavior of positronium is very sensitive to the dispersion state of NiO on the surface of γ-Al(2)O(3). When the NiO loading is lower than monolayer dispersion capacity, spin conversion of positronium induced by NiO is the dominant effect, which causes decrease of the longest lifetime and its intensity but increase of the narrow component intensity. After the NiO loading is higher than monolayer dispersion capacity, the spin conversion effect becomes weaker and inhibition of positronium formation by NiO is strengthened, which results in decrease of both the long lifetime intensity and the narrow component intensity. The reaction rate constant is determined to be (1.50 ± 0.04) × 10(10) g mol(-1) s(-1) and (3.43 ± 0.20) × 10(9) g mol(-1) s(-1) for NiO content below and above monolayer dispersion capacity, respectively.     

Formation of NiO/YSZ functional anode layers of solid oxide fuel cells by magnetron sputtering

The decrease in the polarization resistance of the anode of solid-oxide fuel cells (SOFCs) due to the formation of an additional NiO/(ZrO₂ + 10 mol % Y₂O₃) (YSZ) functional layer was studied. NiO/YSZ films with different NiO contents were deposited by reactive magnetron sputtering of Ni and Zr–Y targets. The elemental and phase composition of the films was adjusted by regulating oxygen flow rate during the sputtering. The resulting films were studied by scanning electron microscopy and X-ray diffractometry. Comparative tests of planar SOFCs with a NiO/YSZ anode support, NiO/YSZ functional nanostructured anode layer, YSZ electrolyte, and La_0.6Sr_0.4Co_0.2Fe_0.8O₃/Ce_0.9Gd_0.1O₂ (LSCF/CGO) cathode were performed. It was shown that the formation of a NiO/YSZ functional nanostructured anode leads to a 15–25% increase in the maximum power density of fuel cells in the working temperature range 500–800°C. The NiO/YSZ nanostructured anode layers lead not only to a reduction of the polarization resistance of the anode, but also to the formation of denser electrolyte films during subsequent magnetron sputtering of electrolyte.     

Magnetron formation of Ni/YSZ anodes of solid oxide fuel cells

Physico-chemical and structural properties of nanocomposite NiO/ZrO₂:Y₂O₃ (NiO/YSZ) films applied using the reactive magnetron deposition technique are studied for application as anodes of solid oxide fuel cells. The effect of oxygen consumption and magnetron power on the discharge parameters is determined to find the optimum conditions of reactive deposition. The conditions for deposition of NiO/YSZ films, under which the deposition rate is maximum (12 μm/h), are found and the volume content of Ni is within the range of 40–50%. Ni-YSZ films reduced in a hydrogen atmosphere at the temperature of 800°C have a nanoporous structure. However, massive nickel agglomerates are formed in the course of reduction on the film surface; their amount grows at an increase in Ni content in the film. Solid oxide fuel cells with YSZ supporting electrolyte and a LaSrMnO₃ cathode are manufactured to study electrochemical properties of NiO/YSZ films. It is shown that fuel cells with a nanocomposite NiO/YSZ anode applied using a magnetron sputtering technique have the maximum power density twice higher than in the case of fuel cells with an anode formed using the high-temperature sintering technique owing to a more developed gas-anode-electrolyte three-phase boundary.     

Synthesis and Characterization of High-purity Aluminum Titanate with Water Quenching Method

High-purity aluminum titanate was synthesized via a water quenching method with waste-residue in the aluminum factory and industrial TiO2 as the main raw materials, which belongs to the comprehensive utilization of solid wastes. Compared with the conventional method, it can reduce synthesis temperature, effectively inhibit decomposition and raise the content of AT; the addition of tiny silicon powder can improve the sintering and optimize the properties of AT. The crystalline phase structure and microstructure of each sample were characterized with XRD and SEM methods; the content of each crystalline phase in each sample was confirmed with Rietveld Quantification method; the properties of each sample were also tested. The experimental results showed that No. 4 is the optimum specimen, with the corresponding mass ratio of Al2O3/TiO2 to be 1.27 and the content of AT of 97.2 wt%. The addition of optimum tiny silicon powder is confirmed to be 8wt%; its corresponding bulk density is 2.63 g/cm^3, bending strength is 46.34 MPa, and the retention of one thermal vibration bending strength is 71.5%.     

水热法制备Ni/ Zr0.4Ce0.6O2-Al2O3催化剂上CH4-CO2重整反应研究: NiO含量的影响

采用水热合成法制备不同NiO含量的Ni/Zr0.4Ce0.6O2-Al2O3催化剂，使用X射线衍射（XPD）和H2的程序升温还原（H2-TPR）对样品进行表征，研究了NiO的含量对催化剂结构和CH4-CO2重整性能的影响。结果表征表明，少量Ni组分能在催化剂表面分散并进入CeO2-ZrO2固熔体晶格间隙而被固熔体包裹，并使固熔体晶粒变小，促进了固熔体的低温还原，而过量的NiO暴露在外生成NiO颗粒。活性测试结果表明，NiO含量少的样品活性随反应进行有较高的增长。选择适当空速，能使CH4-CO2以1：1反应。