双极谱峰指示催化动力学极谱法测定痕量钒

在硫酸介质中,以酒石酸为活性剂,痕量钡对溴酸钾氧化乙基橙的反应具有极强的催化作用,研究了最佳反应条件,且发现在氨性缓冲溶液中乙基橙及其氧化产物具有良好的极谱峰,以极谱法监测催化反应过程中乙基橙及其氧化产物浓度的变化,建立了催化动力学极谱法测定痕量钒的新方法,方法的线性范围为０．２５～３．５０ｕｇ／Ｌ,检出限为０．１２ｕｇ／Ｌ。应用于食品中痕量钒的测定,结果满意。     

催化反应-示波极谱法测定痕量钒

在硫酸介质及100℃水浴加热条件下,钒(Ⅴ)对过硫酸铵氧化二苯羟乙酸生成二苯甲酮这一慢反应具有强烈的催化作用,据此拟定了一个测定8.0～100ng/ml钒的催化反应-示波极谱法,并用于测定铝合金及纯铝中钒的含量。     

催化动力学极谱法测定痕量钒

在硫酸介质中,以酒石酸为活化剂,痕量钒对溴酸钾氧化甲基橙的反应有极强的催化作用,以极谱法监测催化反应过程中甲基橙及其氧化产物浓度的变化,建立了双峰指示催化动力学极谱法制定痕量钒的新方法,方法的线性范围为0.23-3.70μg/L,检出限为0.17μg/L。方法已用于食品及水样中痕量钒的测定。     

催化动力学极谱法测定痕量钼

在稀Ｈ２ＳＯ４介质中，钼（Ⅵ）对硫酸联氨还原乙基橙的反应有强烈的催化作用。建立了催化动力学极谱法测定痕量钼的新体系，方法线性范围为２０－３００ｎｇ／ｍＬ，检出限为３．５４ｎｇ／ｍＬ。方法应用于尿中中钼的测定，结果满意。     

催化动力学极谱法测定痕量钒

1 引言 本文基于在酸性条件下,钒对氯酸钾氧化对硝基苯肼成偶氮离子,继与变色酸偶联反应的催化作用,利用极谱仪器监测反应过程中对硝基苯肼浓度的变化,建立了催化动力学极谱法测定钒的新方法。方法具有线性范围宽,分析速度快,选择性好和灵敏度高等优点。     

溴酸钾氧化酸性铬深蓝催化动力学极谱法测定痕量钒

在0.15mol·L~(-1)H_2SO_4介质中,以酒石酸作活化剂,Ⅴ(Ⅴ)对溴酸钾氧化酸性铬深蓝的反应具有强烈的催化作用,以极谱法监测催化反应过程中酸性铬深蓝浓度的变化,建立了测定痕量钒的催化动力学新方法。钒的线性范围为0.10～7.0ng·ml~(-1),检出限为0.05ng·ml~(-1),应用于人发中痕量钒的测定,结果满意。并对酸性铬深蓝的极谱特性进行了初步的探讨。     

催化动力学极谱法测定痕量甲醛

在稀硫酸介质中,痕量甲醛对溴酸钾氧化甲基红的反应有很强的催化作用.而甲基红及其氧化产物均能在滴汞电极上产生灵敏的极谱吸附波,其峰电位依次为-0.57 V及-0.49 V(vs.SCE).在-0.57 V处测得的甲基红的峰电流的二阶导数值与反应体系中的甲醛浓度在0.2～6.5 mg·L-1之间呈线性关系,方法的检出限为0.041 mg·L-1,对2.5 mg·L-1甲醛测定8次,得出RSD值为1.8%,标准加入法回收率试验的结果在97.0%～104.0%之间.     

催化动力学极谱法测定痕量亚硝酸根

在硫酸介质中，痕量亚硝酸根对溴酸钾氧化酸性铬深蓝的反应有极强的催化作用，研究了最佳反应条件，发现在氨缓冲溶液中酸性铬深蓝具有良好的极谱峰，以极变法监测催化反应过程中酸性铬深蓝浓度的变化，建立了催化动力学极谱法测定痕量亚硝酸根的方法，方法的线性范围为0．20－1．34μg.ml^-1，检出限为0．088μg.ml^-1，应用于雪水，雨水中痕量亚硝酸根的测定，结果满意。     

极谱催化波法测定地塞米松

基于地塞米松在过硫酸钾存在下产生的极谱催化波 ,拟定了测定地塞米松的新方法。与基于还原波的差分脉冲极谱法相比 ,本方法用线性变位极谱法获得的分析灵敏度提高了两个数量级。在 2 .0× 10 - 3mol LH2 SO4 ～ 2 .0× 10 - 2 mol LK2 S2 O8底液中 ,地塞米松于 - 1 0 8V (vs .SCE)处产生一极谱催化波 ,其二阶导数峰电流与地塞米松浓度在 3.2× 10 - 8～ 3.2× 10 - 7mol L范围内呈线性关系 (r =0 .9994 ,n =6 ) ,检出限为 1.0×10 - 8mol L。讨论了极谱催化波产生的机理。     

极谱催化波法测定马蔺子素

报道了在Na2 B4 O7 KH2 PO4 K2 S2 O8体系中马蔺子素的极谱催化波。拟定了测定马蔺子素的新方法。在 8.0× 10 - 3mol/LNa2 B4 O7 1.6× 10 - 2 mol/LKH2 PO4 (pH =7.7) 5 .0× 10 - 3mol/LK2 S2 O8底液中 ,极谱催化波峰电位Ep=-1.2 3V(vs .SCE) ;二阶导数峰峰电流i″p 与马蔺子素浓度在 2 .0× 10 - 9～ 2 .0× 10 - 6 mol/L范围内呈良好线性关系 ,检出限为 1.0× 10 - 9mol/L。催化波灵敏度比相应马蔺子素还原波高 75倍。采用该法测定了胶囊中马蔺子素的含量     

多目标单纯形法在茜素红催化荧光测定痕量钒(V)中的应用

本文建立了茜素红催化荧光测定痕量钒(V)的新方法.在λ_(ex)/λ_(em)=381/445(nm),由多目标罚函数单纯形法获得最佳实验条件为:1%茜素红6mL,1mol/L盐酸2.1mL,饱和KIO_4,1.8mL,反应温度85℃,反应时间15.30min,钒的检测下限为7×10~(-10)g/mL,反应对试剂及金属离子均为一级反应.方法用于水样和铬钒钢中钒的测定,结果满意.     

极谱催化波法测定黄连素

基于黄连素在过氧化氢存在下产生的极谱催化波,拟定了测定黄连素的新方法。在８．０×１０－２ｍｏｌ／ＬＮａ２Ｂ４Ｏ７－Ｎａ２ＣＯ３（ｐＨ９．４±０．４）－４．０×１０－３ｍｏｌ／ＬＨ２Ｏ２底液中,催化波峰电流与黄连素浓度在 １．０ × １０－８～ ３．０ × １０－７ｍｏｌ／Ｌ范围内呈线性关系。催化波的灵敏度比相应黄连素还原波高２５倍。     

全钒液流电池高浓度下V(IV)/V(V)的电极过程研究

采用循环伏安、低速线性扫描和阻抗技术, 以石墨为电极, 研究了V(IV)/V(V)在较高浓度下的电极过程. 结果表明, 采用2.0 mol•L-1 的V(IV)溶液时, H2SO4浓度低于2 mol•L-1, V(IV)/V(V)反应极化大, 可逆性差, 表现为电化学和扩散混合控制; H2SO4浓度增至2 mol•L-1以上, V(IV)/V(V)反应的可逆性提高, 转为扩散控制, 且增加H2SO4浓度有利于阻抗的降低; 但H2SO4浓度超过3 mol•L-1, 溶液的粘度和传质阻力大, 阻抗反而增大. 在3 mol•L-1的H2SO4中, 随着V(IV)浓度的增加, 体系的可逆性和动力学改善, 阻抗减小; 但V(IV)浓度超过2.0 mol•L-1, 较高的溶液粘度导致溶液的传质阻力迅速增加, V(IV)/ V(V)的电化学性能衰减, 阻抗增大. 因此, 综合考虑电极反应动力学和电池的能量密度两因素, V(IV)溶液的最佳浓度为1.5～2.0 mol•L-1, H2SO4浓度为3 mol•L-1.     

Catalytic and kinetic spectrophotometric method for determination of vanadium(V) by 2,3,4-trihydroxyacetophenonephenylhydrazone

A new catalytic and kinetic spectrophotometric method for the determination of vanadium(V) was studied using 2,3,4-trihydroxyacetophenonephenylhydrazone (THAPPH) as an analytical reagent. The present method was developed on the catalytic effect of vanadium on oxidation of THAPPH by hydrogen peroxide in hydrochloric acid–potassium chloride buffer (pH = 2.8) at the 20th minute. The metal ion has formed 1:2 (M:L) complex with THAPPH. Beer’s law was obeyed in the range 20–120 ng/mL of V(V) at λ_max 390 nm. The sensitivity of the method was calculated in terms of molar absorptivity (1.999 × 10⁵ L mol⁻¹cm⁻¹) and Sandell’s sensitivity (0.000254 μg cm⁻²), shows that this method is more sensitive. The standard deviation (0.0022), relative standard deviation (0.56%), confidence limit (±0.0015) and standard error (0.0007) revealed that the developed method has more precision and accuracy. The stability constant was calculated with the help of Asmu’s (9.411 × 10⁻¹¹) and Edmond’s & Birnbaum’s (9.504 × 10⁻¹¹) methods at room temperature. The interfering effect of various cations and anions was also studied. The present method was successfully applied for the determination of vanadium(V) in environmental and alloy samples. The method’s validity was checked by comparing the results obtained with atomic-absorption spectrophotometry and also by evaluation of results using F-test.     

溴酸钾-RB体系催化动力学光度法测定痕量钒

钒是人体不可缺少的微量元素之一,人体中钒含量过高或过低都会影响人体的新陈代谢,从而引起不适应症状甚至病变。钒主要存在于岩石矿物中,钢铁、淤泥、废水、食品甚至于人的头发中也含有微量钒。目前,钒的测定主要有光度法[1]、荧光法[2]、化学发光法[3]、极谱法[4]、色谱法[5]     

Azidokomplexe von Vanadium(IV) und Vanadium(V): (Ph4P)2[VOCl2(μ‐N3)]2 und (Ph4P)2[VOCl(μ‐N3)(N3)2]2

Azido Complexes of Vanadium(IV) and Vanadium(V): (Ph₄P)₂[VOCl₂(μ‐N₃)]₂ and (Ph₄P)₂[VOCl(μ‐N₃)(N₃)₂]₂ (Ph₄P)₂[VOCl₂(μ‐N₃)]₂ ( 1 ) was prepared by reaction of (Ph₄P)[VO₂Cl₂] with trimethylsilylazide in the molar ratio 1:2 in dichloromethane solution to give dark green, moisture sensitive, non‐explosive single crystals. The reaction is accompanied by the formation of the dark blue side‐product (Ph₄P)₂[VOCl(μ‐N₃)(N₃)₂]₂ ( 2a ), which can be obtained as the main product by application of a large excess of Me₃SiN₃. Dark blue needles of 2a crystallize spontaneously from the CH₂Cl₂ solution within one hour at 4 °C. After standing at 4 °C under its mother liquid within 24 hours a first‐order phase transition of 2a occurs forming dark blue prismatic single crystals of 2b . According to single crystal X‐ray structure determinations, 2a and 2b crystallize in the same type of space group , however, with different lattice dimensions. The vanadium(IV) complex 1 is characterized by X‐ray structure determination and by vibrational spectroscopy (IR, Raman) as well as by EPR spectroscopy, whereas 2b is characterized by IR spectroscopy. 1 : Space group P2₁/n, Z = 2, a = 1009.5(1), b = 1226.6(2), c = 1943.0(2) pm, β = 98.42(1)°, R₁ = 0.0672. The complex anion forms centrosymmetric units with V₂N₂‐four‐membered rings with a V···V distance of 335.6(1) pm and coordination number five on the vanadium(IV) atoms. 2a : Space group , Z = 1, a = 1089.0(2), b = 1097.1(2), c = 1310.1(2) pm, α = 92.99(1)°, β = 106.12(2)°, γ = 117.05(2)°, V = 1309.8(4) ų, d_calc. = 1.440 g·cm^?3, R₁ = 0.0384. The complex anion forms centrosymmetric units of symmetry C_i with V₂N₂ four‐membered rings and VN bond lengths of 200.4(3) and 234.4(2) pm, respectively. The non‐bonding V···V distance amounts to 356.2(1) pm. 2b : Space group , Z = 1, a = 1037.3(2), b = 1157.6(2), c = 1177.2(2) pm, α = 98.48(2)°, ° = 103.82(2)°, γ = 106.33(2)°, V = 1281.8(4) ų, d_calc. = 1.471 g·cm^?3, R₁ = 0.0724. The structure of the complex anion is similar to the anion of 2a with VN bond lengths of the four‐membered V₂N₂ ring of 203.3(4) and 235.2(4) pm, respectively, and a non‐bonding V···V distance of 357.5(1) pm.