ICP-AES测定葡萄糖酸钙中Pb、As、Cd等9个杂质元素

本文应用ICP-AES直接测定了葡萄糖酸钙中的Pb、As、Cd等9个杂质元素,对样品的消解方法、基体和酸介质的影响等进行了讨论.用基体匹配法消除钙基体的干扰,9个杂质元素测定的测定范围为:Pb 0.0008%-0.08%,Cu、Mg 0.0001%-0.01%,其余元素0.0003%-0.03%.加标回收率为95.8%-100.0%,相对标准偏差为0.16%-3.61%.     

ICP-AES测定铝合金中Mg、Be、Mn、Mo、Fe、Ti、Si和Zn

采用ICP-AES同时测定铝合金中合金元素和杂质元素,优化ICP光谱仪的工作条件,测定回收率96%-106%.RSD 0.28%-6.26%,结果令人满意.     

ICP-MS测定碳酸锂中微量元素

用ICP-MS测定碳酸锂中微量杂质元素的基本条件,确定了合适的样品处理、分解方法,研究了元素间的干扰.方法检出限K0.020μg/g,Na o.025μg/g,Ca0.009μg/g,Mg 0.010μg/g,SO2-4 0.050μg/g;加标回收率在94.0%-102.0%,测定精密度RSD 0.5%-2.1%,方...     

ICP-AES法同时测定银锭中铋、锑、铅、铜、铁杂质元素

本文介绍ICP-AES法同时测定银锭中Bi、Sb、Pb、Cu、Fe杂质元素的方法。试样用稀硝酸溶解后测定,回收率为93.0%-105.0%,RSD为0.36-4.2%。     

ICP-AES法直接测定锡锭中的As、Al、Bi、Cd、Cu、Fe、Pb、Se、Sb、Zn

以电荷耦合器件为检测器的全谱直读等离子体光谱仪直接测定锡锭中As、Al、Bi、Cd、Cu、Fe、Pb、Se、Sb、Zn十种杂质元素的含量.该方法简便、快速且具有比化学法更低的检出限,加标回收试验结果表明,回收率为92%-105%,RSD均小于1.5%.     

电感耦合等离子体-原子发射光谱法测定新锆合金(锆-锡-铁-铬-铌)中10种微量杂质元素

IPC-AES测定了新锆合金中10种微量杂质元素Al、Co、Cu、Mg、Mn、Mo、Ni、Pb、Ti和V.试液浓度为10mg/mL时,测定范围在20-1060μg/g之间,回收率在94%-108%之间,相对标准偏差(RSD,n=6)为4.3%-7.4%之间.     

火焰原子吸收法测定氰化镀银液中的铜和铁

提出了用火焰原子吸收光谱法测定氰化镀银液中铜、铁含量的方法,在测定条件下,其他共存元素均无干扰。该方法的相对标准偏差为铜（1.92%-2.63%、铁3.13%-3.73%,样品加标回收率为铜96.8%-101.6%、铁97.5%-101.1％。     

原子吸收光谱法测定电解金属锰中微量金属杂质元素

本文用盐酸溶解样品,火焰原子吸收光谱法测定电解金属锰中K,Na,Ca,Mg,Fe,石墨炉原子吸收光谱法测定其中的Cr,Cu,Co,Ni含量。对测定条件进行了实验,找出最佳溶样方法和酸度,对共存元素的干扰有排除亦进行了试验,获得了满意的效果。该法简便、快速、准确,加标回收率为88.9%-108.7%之间,相对标准偏差为0.6%-6.7%,标准曲线法、标准加入法结果与对照结果相吻合,适用于电解金属锰样品金属杂质元素的分析。     

ICP-AES同时测定南极石中的22种元素

电感耦合等离子体原子发射光谱法(ICP-AES)同时测定南极石中的铜、铁、锌、钙、镁、锰、钴等22种元素的含量.优化了消解样品用酸,选择了适合的元素分析线.各元素测定的相对标准偏差为0.13%-5.14%,加标回收率为95.43%-108.68%,方法简单、可靠,具有良好的准确度和精密度.     

氢化物发生-原子荧光光谱法测定铜阳极泥中的砷

用氢化物发生-原子荧光光谱法测定铜阳极泥中的砷量,研究了仪器测量条件、氢化物发生条件、共存元素等因素对测定结果的影响.选择了最佳测定条件,砷的测定范围为0.50%-5.00%,加标回收率在98.3%-108.0%之间,相对标准偏差小于4%,能满足测定的要求.     

用扫描式电感耦合等离子体光谱仪测定红矾钾产品中的杂质

应用电感耦合等离子体发射光谱法测定了铬盐清洁工艺红矾钾产品中的微量元素硅、铝、铁、钙、锰、镁和氯。采用基体匹配法消除了大量基体的干扰。实验的优化条件为RF发生器的入射功率095kW;载气压力013MPa,流量12L·min-1;辅助气流量02L·min-1。元素氯用氯化银沉淀间接测定,在6%的硝酸体系中氯离子形成氯化物完全沉淀,在50℃陈化2h后进行测定。样品的加标回收率在90%～104%,RSD<4%,检出限在10-4%～10-5%。随机抽样的分析结果与标准加入法吻合较好,相对误差在-427%～ 526%。本方法用于实际样品分析,快速简单,结果令人满意。     

HEH[EHP]萃取色层分离-原子发射光谱测定超高纯氧化钬、氧化铒中痕量稀土杂质

本文研究了２－乙基己基膦酸单２－乙基己酯萃取色层分离－原子发射光谱测定超高纯Ｈｏ２Ｏ３、Ｅｒ２Ｏ３中良量稀土杂质,可用于９９．９９９９％Ｈｏ２Ｏ３、Ｅｒ２Ｏ３的纯度分析。     

氯化钯作基体改进剂GFAAS法测定中药材中微量铅的研究

建立了氯化钯作基体改进剂,石墨炉原子吸收测定中药材中微量铅的方法.对氯化钯用量、介质酸度、共存离子干扰及方法回收率、精密度、检出限进行了考查.氯化钯作基体改进剂对铅的改进效果优于磷酸二氢铵.方法回收率为90%～104%,精密度(RSD)＜5.0%,特征质量为8.5 pg,检出限为0.066 mg·kg-1.方法简单、灵敏、准确、可靠,值得推广.     

一套红外池测定精四氯化钛中二氯氧钛的含量

钛材质量控制的关键是控制精TiCl₄中杂质含量。精TiCl₄是海绵钛生产的关键环节,海绵钛中杂质与精TiCl₄中杂质含量成4倍富集关系。需要分析氧杂质的来源,对精TiCl₄中氧杂质进行严格控制。精TiCl₄中TiOCl₂含量的测定具有重要意义。TiOCl₂具有红外吸收谱线,因而能够利用红外光谱实现测定,然而精TiCl₄与空气中水气接触极易发生水解反应,生成强腐蚀性的盐酸烟雾,不能使用常规的红外吸收池进行测定。根据Lambert-Beer定律,被测组分浓度(c_x)与吸光度(A)～样品光程(L)曲线的斜率成正比,利用波长范围7 800～440 cm-1的硒化锌窗片(10×1 mm)和玻璃池体(22,12,7和4 mm光程)组装成一套红外吸收池,采用加标法测定精TiCl₄中TiOCl₂杂质含量。实验得出TiOCl₂的检出限为17.8 mg·kg-1,样品回归方程Y=1.0118X,相关系数r为0.996 3,加标TiOCl₂样品的回归方程Y=1.940 0X,相关系数r为0.997 0,线性关系较好。测定精TiCl₄中TiOCl₂含量为833.8 mg·kg-1,标准偏差(SD)为40.0 mg·kg-1,方法精密度相对标准偏差(RSD)在0.95～1.94之间,加标回收率在88.5%～93.1%之间。此红外吸收池安全简便、容易拆洗、可重复使用,通过一次加标样品定量分析精TiCl₄中TiOCl₂含量,可满足精TiCl₄中TiOCl₂分析的要求。     

Cu(In,Ga)Se2 thin-film solar cells with ZnS(O,OH), Zn-Cd-S(O,OH), and CdS buffer layers

Cu(In,Ga)Se₂ (CIGS) solar cell junctions prepared by chemical-bath-deposited (CBD) ZnS(O,OH), Zn-Cd-S(O,OH), and CdS buffer layers are discussed in this paper. The device performances are compared by applying CBD ZnS(O,OH), CBD Zn-Cd-S(O,OH), and CBD CdS buffer layers on similar CIGS absorbers. The CN impurities in CBD ZnS(O,OH) are identified with Fourier transform infrared spectroscopy (FTIR) techniques. The impurities containing carbon-nitrogen bonds are most likely cyanamide (NCN²⁻) or thiocyanate (SCN⁻), which resulted from the chemical reaction of thiourea and ammonia.     

Deuteron spin-lattice relaxation in partly and fully deuterated (NH(4))(2)PdCl(6)

Deuteron spin-lattice relaxation and spectra were studied in partially and fully deuterated (NH(4))(2)PdCl(6) in the temperature range 5-300K. The relaxation rate maximum was observed at 45K in (ND(4))(2)PdCl(6). Its value is reduced due to limited jumps by about 33% relative to the theoretical value expected for threefold reorientations. Limited jumps correspond to an N-D vector jumping between six directions on a cone around a Pd-N vector, the angle between the N-D and Pd-N vectors being denoted Delta. This motion makes a part of the quadrupole interaction ineffective in relaxation thus reducing the maximum rate at 45K. The observed reduction leads to the value Delta=21( composite function). Limited jumps are quenched to a large extent at the order-disorder phase transition and consequently a decrease is observed in the rate. Below the transition ND(4)(+) ions reorient between the tetrahedral orientations of the ordered phase, therefore the quadrupole interaction has the full relaxing efficiency. In the 10% deuterated sample the temperature of the rate maximum is shifted to 35K and below 20K the rate itself is one order of magnitude larger than in (ND(4))(2)PdCl(6). The increase is related to (1) the absence of the order-disorder phase transition and (2) to the enhanced mobility of NH(3)D(+) because of its electric dipole moment. Limited jumps are claimed to be the dominant relaxation mechanism below 20K. The relaxation in the disordered 30% deuterated sample is quite similar to that in 10% sample. The 50% and 70% deuterated samples undergo a transition to the ordered phase. The relaxation is biexponential with the characteristic rates somewhat smaller than those in (ND(4))(2)PdCl(6), but approaching them with increasing deuteration. This variation can be explained with different mobilities and varying relative numbers of the various isotopomers NH(4-n)D(n)(+), n=1-4.     

石墨炉原子吸收光谱法测定中成药中砷,铅

本文以HNO3 HClO4 为氧化剂 ,压力消解处理样品 ,氯化钯作测砷基体改进剂 ,磷酸氢二铵作测铅基体改进剂 ,考察了基体改进剂用量、灰化温度、原子化温度以及干扰元素对测定的影响 ,在最佳测定条件下 ,用石墨炉原子吸收光谱法测定了中成药中砷和铅 ,砷和铅测试结果分别为 :线性范围为 0～ 30 0ng·mL-1和 0～ 80ng·mL-1,检测限 3 75ng·mL-1和 1 8ng·mL-1,灵敏度 9 3ng·mL-1和 2 6ng·mL-1,平均回收率 95 7%和99 6 %。方法简单 ,灵敏度高 ,重现性好。     

PdCl_2/SiO_2和Pd-B/SiO_2非晶态合金催化剂的Raman光谱表征

采用共焦显微Ｒａｍａｎ光谱和Ｘ－射线衍射方法表征了负载型ＰｄＣｌ２／ＳｉＯ２和Ｐｄ－Ｂ／ＳｉＯ２非晶态合金催化剂的结构。结果表明ＰｄＣｌ２分散在ＳｉＯ２载体上后,与载体表面的相互作用使其在室温时即发生β→α构型转变。Ｐｄ－Ｂ／ＳｉＯ２非晶态合金的Ｒａｍａｎ光谱在３００－５００ｃｍ－１区域内呈现一大的弥散峰。与无负载Ｐｄ－Ｂ非晶态合金比较初步认定该弥散峰与Ｐｄ－Ｂ键振动有关,温度升高Ｐｄ－Ｂ／ＳｉＯ２催化活性下降,其主要原因为Ｐｄ－Ｂ／ＳｉＯ２非晶态合金在高温下逐渐晶化为Ｐｄ金属所致。ＰｄＣｌ２与ＳｉＯ２载体表面的相互作用使其具有较高的分散性,由此还原制备的Ｐｄ－Ｂ／ＳｉＯ２非晶态合金较之无负载Ｐｄ－Ｂ非晶态合金更加微细化,因而具有更大的活性比表面     

电感耦合等离子体发射光谱法测定氧化钐中非稀土杂质铜,铁, …

本文提出了用ＩＣＰ－ＡＥＳ法直接测定高纯氧化钐中痕量杂质铜、铁、钙和镍的方法。用正交实验法研究了影响测定的主要因素，选择了铜、铁、钙和镍同时测定的折衰条件。讨论了基体浓度的影响。     

Synthesis of original spherical α-Ni(OH)2 architectures by microwave-assisted hydrothermal method and their in situ thermal convention to NiO

The original spherical α-Ni(OH)₂ architectures with many cubic particles growing from the surface were successfully synthesized by a microwave-assisted hydrothermal method using urea as hydrolysis-controlling agent and polyethylene glycol (PEG) as surfactant. The NiO architectures with similar morphology were obtained by simple thermal decomposition of the precursor α-Ni(OH)₂. The as-obtained products were well characterized by XRD, FTIR, TGA, SEM, TEM, UV–Vis and CVs. The experimental results showed that the diameter of spherical α-Ni(OH)₂ architectures was in the range of 2–4 μm. The side length of the cubic particles was uniform about 200 nm. The cyclic voltammetric results showed that the reversible behavior of NiO electrode change better with the increasing of the cycle index. The original NiO we have prepared are expected to have good electrochemical behavior.