用计时电位法测定镧在铝液中的扩散系数

采用新的阳极溶解的计时电位法,测定了稀土金属镧在铝液中的扩散系数。在973K时,测得(Al)=(1.21±0.02)×15~(5)cm~2·s~(-1)。在953～1053K温度范围内,扩散系数与温度的关系为lgD_(La)(Al)=1.04×10~(-4)—4770/T,计算出扩散激活能Q=91.34KJ/mol。     

抗坏血酸在普鲁士蓝薄膜修饰电极上的电催化氧化

本文详细研究了普鲁士蓝(PB)薄膜本身电荷传输过程的动力学及PB 薄膜催化抗坏血酸(AH2)电氧化的动力学。 用电位阶跃计时电流法和计时电量法, 恒电流计时电位法测得PB膜中电荷传输表观扩散系数Dct平均为2.62×10ˉ10cm2·sˉ1; 用RDE法测得AH2在PB薄膜上催化氧化的速率常数为1.23×10^8cm3·molˉ1·sˉ1。催化反应对AH2为一级。 只发生在PB薄膜与溶液的界面上。 整个催化过程受到溶液中的传质、膜内部的电荷传输及膜与溶液界面上交叉反应三种因素单独或联合控制, 实际出现四种动力学情况。     

新型锂离子电池阳极材料Li2.7Mg0.3N的研究

以氮化锂和镁金属为原料,制备了Li2.7Mg0.3N样品,利用XRD、原子吸收、库仑滴定等方法研究了锂离子电池阳极材料Li2.7Mg0.3N的组成、结构及电化学性能。样品Li2.7Mg0.3N经成分分析组成为Li2.74Mg0.26N;其结构为四方晶系,晶胞参数a=0.388nm,c=0.547nm;比容量为1695(mA.h)/g,嵌入量x最大可达2.5276,室温时锂离子嵌入Li2.7Mg0.3N的嵌入自由能为-397.51kJ/mol,锂离子在Li2.7Mg0.3N中的化学扩散系数为5.90×10^-^11～7.23×10^-^10cm^2/s,并得到一系列热力学和动力学参数。     

青蒿素及其衍生物电化学性质的研究I. 青蒿素在汞电极上的电化学还原

青蒿素及其衍生物代表着一类新型抗疟药。青蒿素分子中过氧基与抗疟活性密切相关。本文采用多种电化学方法研究了青蒿素分子中过氧基在Hg电极上的还原, 还原电位在0.0V(vs.Ag/AgCl)附近, 电极过程为不可逆还原, 反应电子数n=2, 半波电位E1/2=0.012V, 电子转移系数α=0.66, 表观标准电极反应速率常数ks'=6.34×10^-^6cm/s, 扩散系数D=4.3×10^-^6cm^2/s。反应产物在电极表面具有吸附性, 文中提出了可能的电化学反应机理。     

锂在非层状硫化物中的电化学嵌入反应I:锂在硫化铅中的嵌入过程

通过库伦滴定、三角波电位扫描和X射线衍射物相分析,研究了Li/PbS电池的阴极反应机理.发现在该电池放电的第一个阶段(放电深度小于1.5),阴极上发生的是锂嵌入硫化铅晶格的反应,并且锂嵌入后硫化铅的主晶格结构基本未变,锂进入了晶体的立方体间隙中心位置.测得锂嵌入硫化铅生成LiPbS的嵌入自由能为-300.48kJ.mol^-^1(25℃),锂在LiyPbS(0相似文献   

纳米MgO掺杂改善LiNi1/3Co1/3Mn1/3O2正极材料

将氢氧化物共沉淀法制备的(Ni_1/3Co_1/3Mn_1/3)（OH）₂在500℃热处理5 h得到具有尖晶石结构、纳米尺寸的氧化物M₃O₄(M=Ni_1/3Co_1/3Mn_1/3).将其与LiOH及不同量的纳米MgO混合均匀,并在850℃热处理24 h制备了Li(Ni_1/3Co_1/3Mn_1/3)_1/xMg_xO₂（x=0,0.01,0.02,0.03,0.04,0.05）正极村料.随着Mg掺杂量的增大,正极材料的晶胞参数增大;少量的Mg掺杂增大了锂离子的扩散系数,而过度掺杂却使锂离子扩散系数有所降低,其中Li(Ni_1/3Co_1/3Mn_1/3)_0.98Mg_0.02O₂的锂离子扩散系数最大,其脱出和嵌入扩散系数分别为D_Li-dein=29.20×10^-11cm²·S^-1和D_Li-in=4.760×10^-11cm²·s^-1;其以3C倍率充放电的平均放电比容量为139.3 mAh·g^-1,比未掺杂的原粉约高9.5 mAh·g^-1;另外其循环性能也得到了大幅度改善.     

氨基改性Fe_(3)O_(4)纳米材料修饰电极同时测定Cd^(2+)和Pb^(2+)北大核心CSCD

采用溶剂热法一步合成氨基改性的Fe_(2)O_(4)(NH_(2)-Fe_(3)O_(4))纳米材料,通过扫描电镜、红外光谱、X射线衍射等方法对合成纳米材料进行表征,并将NH_(2)-Fe_(3)O_(4)滴涂在玻碳电极(GCE)表面制成电化学传感电极(NH_(2)-Fe_(3)O_(4)/GCE)。结果发现,NH_(2)-Fe_(3)O_(4)/GCE在最优条件下可以同时测定Cd^(2+)和Pb^(2+),Cd^(2+)在1.2×10^(-8)~9.6×10^(-5)mol·L^(-1)浓度范围内与峰电流值呈良好的线性关系(R=0.9949),检测限为1.4×10^(-9)mol·L^(-1);Pb^(2+)在4.8×10^(-8)~9.6×10^(-5)mol·L^(-1)时浓度范围内与峰电流值呈良好的线性关系(R=0.9843),检测限是2.7×10^(-9)mol·L^(-1)。     

百里香酚在聚甲苯胺蓝/多壁碳纳米管修饰电极上的电催化氧化动力学研究

采用电聚合、滴涂及多层修饰方法制备了4种修饰电极,百里香酚在几种修饰电极上均是不可逆电氧化反应,其中聚甲苯胺蓝/多壁碳纳米管修饰电极的电催化效果最佳,过电位降低了111mV,氧化峰电流增大了5倍。在pH为7.69的PBS溶液中,百里香酚在聚甲苯胺蓝/多壁碳纳米管修饰电极上是电子转移数和质子数均为1的扩散控制不可逆电氧化过程,扩散系数D=4.8470×10-4cm2/s,电极有效面积A=0.0383cm2。氧化峰电流ip与浓度c在9.0×10-6～5.0×10-4mol/L范围内呈良好的线性关系:ip(A)=-3.781×10-5-0.0491c(mol/L),相关系数R=-0.9958,样品测定回收率为96.88%～101.50%。     

6-羟基烟酸修饰电极的制备及应用研究

采用循环伏安法制备了6-羟基烟酸膜修饰炭糊电极(6-HNC/CPE),研究了多巴胺(DA)和肾上腺素(EP)在该修饰电极的电化学行为,结果表明该修饰电极对DA及EP具有明显的电催化效果。其电化学信号与DA的浓度在9.52×10-7~7.28×10-5mol·L-1和8.67×10-5~3.72×10-4mol·L-1范围内呈良好的线性关系。检出限为1.9×10-7mol·L-1(S/N=3),氧化峰电流与EP的浓度在1.74×10-6~4.41×10-5mol·L-1和5.58×10-5~1.01×10-4mol·L-1范围内呈良好的线性关系。检出限为3.6×10-7mol·L-1(S/N=3),利用差示脉冲伏安法(DPV),研究DA,UA和Trp的混合溶液电催化效果,结果该发现三者氧化峰电位在6-HNC/CPE上的能够完全分开,该方法操作简单,灵敏度高,可用于三者的选择性测定及实际样品中DA含量的测定。     

trans-[(en)~2(NO~2)Co(O~2CC~5H~5N)]^2^+/Fe(Ⅱ)间电子转移反应动力学及机理研究

合成了新型Co(Ⅲ)配合物trans-[(en)~2(NO~2)Co(O~2CC~5H~5N)](ClO~4)~2, 并通过紫外可见光谱、红外光谱、元素分析和X射线单晶衍射分析进行了表征。同时分别以[Fe(CN)~6]^4^-和[Fe(CN)~5(H~2O)]^3^-作为还原剂, 考察了该配合物被还原的反应动力学行为。结果表明两反应体系分别按外配位界机理和内配位界机理进行电子传递。在25℃, Ⅰ=0.5mol·L^-^1,trans-[(en)~2(NO~2)Co(O~2CC~5H~5N)]^2^+/[Fe(CN)~6]^4^-反应体系的前驱配合物离子对形成常数Q~i~p=29mol^-^1·L, 电子转移速率常数k~e~t=2.4×10^-^4s^-^1,电子转移过程的活化焓△H^≠~e~t和活化熵△S^≠~e~t分别为1.2×10^2kJ·mol^-^1和5.0×10^2J·mol^-^1·K^-^1。在40℃, pH=8.0, Ⅰ=0.1mol·L^-^1,trans-[(en)~2(NO~2)Co(O~2CC~5H~4N)]^2^+/[Fe(CN)~5(H~2O)]^3^-反应体系前驱双核配合物分子内电子转移速率常数为7.0×10^-^5s^-^1。最后讨论了分子轨道对称性, 两金属中心氧化还原电势差等因素对电子转移速率的影响。     

Nafion基氧化还原聚合物在空气中的电荷传输性能

利用三明治电池和伏安法测试了不同制备条件的Nafion基氧化还原聚合物膜在空气中的电荷传输性能. 研究结果表明, 混合适量聚乙二醇(PEG)的Nafion基金属联吡啶配合物{Nafion[M(bpy)2+3, PEG](M=Ru, Fe)}膜的表观电荷传递扩散系数(Dct)达到10-6-10-7 cm2·s-1 , 电子或空穴迁移率(μ)达到10-4-10-5 cm2·V-1·s-1. 在导电玻璃(ITO)电极与Nafion基氧化还原聚合物膜界面引入一层导电聚苯胺(PANI)后, 降低了其接触电阻, 使氧化还原聚合物膜的Dct提高至10-5-10-6 cm2·s-1, μ提高至10-3-10-4 cm2·V-1·s-1, 且工作电流提高了近两个数量级. 该固态氧化还原聚合物膜的性能比较稳定, 在空气中放置30天后其Dct和μ降低得很少.     

Kinetics of the O + HCNO reaction

The kinetics of the O + HCNO reaction were investigated by a relative rate technique using infrared diode laser absorption spectroscopy. Laser photolysis (355 nm) of NO2 was used to produce O atoms, followed by O atom reactions with CS2, NO2, and HCNO, and infrared detection of OCS product from the O + CS2 reaction. Analysis of the experiment data yields a rate constant of k1= (9.84 +/- 3.52) x 10-12 exp[(-195 +/- 120)/T)] (cm3 molecule-1 s-1) over the temperature range 298-375 K, with a value of k1 = (5.32 +/- 0.40) x 10-12 cm3 molecule-1 s-1 at 298 K. Infrared detection of product species indicates that CO producing channels, probably CO + NO + H, dominate the reaction.     

Ab initio studies of ClO(x) reactions: prediction of the rate constants of ClO+NO2 for the forward and reverse processes.

The potential-energy surface for the reaction of ClO with NO2 has been constructed at the CCSD(T)/6-311+G(3df)//B3LYP/6-311+G(3df) level of theory. Six ClNO3 isomers are located; these are ClONO2, pc-ClOONO, pt-ClOONO, OClNO2, pt-OClONO, pc-OClONO, with predicted energies relative to the reactants of -25.6, -0.5, 1.0, 1.9, 12.2 and 13.6 kcal mol-1, and heats of formation at 0 K of 7.8, 32.9, 34.4, 35.5, 45.6 and 47.0 kcal mol-1, respectively. Isomerizations among them are also discussed. The rate constants for the low-energy pathways have been computed by statistical theory calculations. For the association reaction producing exclusively ClONO2, the predicted low- and high-pressure-limit rate constants in N2 for the temperature range of 200-600 K can be represented by: (N2)=3.19 x 10-17 T-5.54 exp(-384 K/T) cm6 molecule-2 s-1 and =3.33 x 10-7 T-1.48 exp(-18 K/T) cm3 molecule-1 s-1. The predicted low- and high-pressure-limit rate constants for the decomposition of ClONO2 in N2 at 200-600 K can be expressed, respectively, by =6.08 x 1013 T-6.54 exp(-13813 K/T) cm3 molecule-1 s-1 and =4.59 x 1023 T-2.43 exp(-13437 K/T) s-1. The predicted values compare satisfactorily with available experimental data. The reverse Cl+NO3 reaction was found to be independent of the pressure, giving exclusively ClO+NO2; the predicted rate constant can be expressed as k(Cl+NO3)=1.19 x 10-9 T-0.60 exp(58 K/T) cm3 molecule-1 s-1..     

Experimental and theoretical study of the electronic spectrum of BeAl

The electronic structure of BeAl was investigated by laser induced fluorescence and resonance enhanced multiphoton ionization spectroscopy. BeAl was formed by pulsed laser ablation of a Be/Al alloy in the presence of helium carrier gas, followed by a free jet expansion into vacuum. In agreement with recent ab initio studies, the molecule was found to have a (2)Pi(1/2) ground state. Transitions to two low lying electronic states, (2)(2)Pi(1/2)(v') <-- X (2)Pi(1/2) (v' = 0) and (1)(2)Delta(v') <-- X (2)Pi(1/2) (v' = 0,1), were observed and rotationally analyzed. An additional band system, identified as (4)(2)Sigma(+)(v') <-- X (2)Pi(1/2), was found in the 28 000-30 100 cm(-1) energy range. This transition exhibited an unusual pattern of vibrational levels resulting from an avoided crossing with the (5)(2)Sigma(+) electronic state. New multi-reference configuration interaction calculations were carried out to facilitate the interpretation of the UV bands.An ionization energy of 48 124(80) cm(-1) was determined for BeAl from photoionization efficiency (PIE) measurements. Fine structure in the PIE curve was attributed to resonances with Rydberg series correlating with vibrationally excited states of the BeAl(+) ion. Analysis of this structure yielded a vibrational frequency of 240(20) cm(-1) for the cation.     

Room temperature and shock tube study of the reaction HCO+O2 using the photolysis of glyoxal as an efficient HCO source

The rate of the reaction 1, HCO+O2-->HO2+CO, has been determined (i) at room temperature using a slow flow reactor setup (20 mbarH2+HCO+CO, into additional HCO radicals. The rate constants of reaction 4 were determined from unperturbed photolysis experiments to be k4(295 K)=(3.6+/-0.3)x10(10) cm3 mol-1 s-1 and k4(769-1107 K)=5.4x10(13)exp(-18 kJ mol-1/RT) cm3 mol-1 s-1(Delta log k4=+/-0.12).     

Association reactions at low pressure. III. The C2H2+/C2H2 system

The association reactions, C4H2(+) + C2H2 and C4H3(+) + C2H2 have been examined at pressures between 8 x 10(-8) and 1 x 10(-4) Torr at 298 K in an ion cyclotron resonance mass spectrometer. Association occurred via two different mechanisms. At pressures below approximately 2 x 10(-6) Torr, the association was bimolecular having rate coefficients k2 = 2.7 x 10(-10) cm3 s-1 and 2.0 x 10(-10) cm3 s-1 for C4H2+ and C4H3+, respectively. At pressures above approximately 2 x 10(-6) Torr, termolecular association was observed with rate coefficients, k3 = 5.7 x 10(-23) cm6 s-1 and 1.3 x 10(-23) cm6 s-1 for C4H2+ and C4H3+, respectively, when M = C2H2. The termolecular rate constants with N2, Ar, Ne, and He as the third body, M, are also reported. We propose that the low pressure bimolecular association process was the result of radiative stabilization of the complex and the termolecular association process was the result of collisional stabilization. Elementary rate coefficients were obtained and the lifetime of the collision complex was > or = 57 microseconds for (C6H4+)* and > or = 18 microseconds for (C6H5+)*. At pressures below 1 x 10(-6) Torr, approximately 11% of the (C6H4+)* were stabilized by photon emission and the remaining approximately 89% reverted back to reactants, while approximately 24% of the (C6H5+)* were stabilized by photon emission and the remaining approximately 76% reverted back to reactants. The ionic products of the C2H2(+) + C2H2 reaction, C4H2+ and C4H3+, were found to be formed with enough internal energy that they did not react by the radiative association channel until relaxed by several nonreactive collisions with the bath gas.     

Determination of Proton Diffusion Coefficient in Spherical Nickel Hydroxide Using Potential Step Measurement on Single Beads

The Potential step measurements are carried out on single beads of nickel hydroxide and the results are interpreted with a dual structure model featuring fast and slow diffusing components The intrinsic diffusion coefficients for the two components are found to be in the order of magnitude 10^-7 and 10^-13-10^-14 cm^2s^-1, respectively, with an apparent value for the slow component in the order of 10^-10 cm^2s^-1.     

含硒杂环萘二酰亚胺衍生物的合成及其场效应性能研究

萘二酰亚胺(NDI)类化合物由于其较好的平面性和较强的接受电子能力,被广泛应用于有机场效应晶体管(OFETs)和有机太阳能电池中(OSCs)。然而,高迁移率的n型和双极性NDI类半导体材料较少。基于此,本文设计合成了核位硒杂环修饰的NDI衍生物,通过引入1,2-二硒苯和1,2-二硒萘基团,对其能级进行了有效的调控,获得了两个新型的窄带隙NDI衍生物。通过溶液旋涂法,制备了两种材料的底栅底接触场效应晶体管器件,二者在空气中都表现出n型半导体特性,退火温度为120℃时性能达到最优,分别为1×10~(-3)cm~2·V~(-1)·s~(-1)(4)和5×10~(-3)cm~2·V~(-1)·s~(-1)(5)。同时,通过原子力显微镜和X射线衍射对材料薄膜的退火过程进行了研究。     

Cross sections and rate constants for the C(3P)+OH(X 2Pi)-->CO(X 1Sigma+)+H(2S) reaction using a quasiclassical trajectory method

First quasiclassical trajectory calculations have been carried out for the C(3P)+OH(X 2Pi)-->CO(X 1Sigma+)+H(2S) reaction using a recent ab initio potential energy surface for the ground electronic state, X 2A', of HCO/COH. Total and state-specific integral cross sections have been determined for a wide range of collision energies (0.001-1 eV). Then, thermal and state-specific rate constants have been calculated in the 1-500 K temperature range. The thermal rate constant varies from 1.78x10(-10) cm3 s-1 at 1 K down to 5.96x10(-11) cm3 s-1 at 500 K with a maximum value of 3.39x10(-10) cm3 s-1 obtained at 7 K. Cross sections and rate constants are found to be almost independent of the rovibrational state of OH.     

尖晶石Li4Ti5O12中锂离子的化学扩散系数的研究

A relatively simple galvanostatic method was used for the evaluation on the average chemical diffusion coefficient of lithium-ion in spinel Li₄Ti₅O₁₂ prepared by solid-state reaction technique. The diffusion coefficient of lithium-ion was estimated to be 2.8×10^-13 cm²·s^-1 and 1.3×10^-13 cm²·s^-1 for charge and discharge， respectively.