石墨炉原子吸收法直接测定高温合金中硅

研究了混合基体改进剂，灰北、原子化温度以及共存元素的干扰，采用镧和钙作混合基体改进剂后，硅的灵敏度提高，抗干扰能力增强，可以用石墨炉原子吸收直接测定高温合多中硅。方法特征量为０．２ｎｇ，检出限为２．３μｇ／ｇ，对于含硅量为４００μｇ／ｇ左右的合金样品，相对标准偏差为５％左右，回收率在９０％－１１０％之间。     

磷钒钼黄差示分光光度法测定阳图 PS 版显影液中的磷

建立了一种与高倍硅共存的磷的分析方法,共存硅对磷钒钼黄色体系的干扰程度与反应介质中硝酸浓度有关,介质中浓度为０．７４ｍｏｌ／Ｌ的硝酸可有效抑制３１倍量的共存硅的干扰。在稀硝酸中煮解,可将六偏磷酸钠转化成正磷酸。     

原子吸收法测定含铜物料中的铂和钯

据文献介绍,在空气-乙炔火焰中测定铂时,锂、钠、钾、钙、镁、铜等元素均能使铂的灵敏度降低,若溶液中含有2毫克镧/毫升并维持0.1M盐酸酸度,可抑制上述干扰。我们在测定冶金中间产品含铜物料中的铂和钯时,发现铜对铂的测定有明显的增敏作用,在试验的     

掺氧空气-乙炔火焰原子吸收光谱法测定钢样中的硅

报道了一种新型掺氧空气-乙炔火焰原子吸收光谱法测定钢中硅的简便方法。当空气流量为6.0 L/min,氧气流量为4.2 L/min,乙炔流量为7.4 L/min时对硅有较高的灵敏度。常见金属离子对硅的测定干扰少。方法的检出限(3σ)为0.85 mg/L,应用于冶金标准管理钢样中的微量硅的测定,结果与标准值相符。对225#碳素钢测定6次,其RSD为3.80%。     

用N2O-C2H2火焰原子吸收光谱法测定膨胀合金中硅

采用N2O-C2H2火焰原子吸收光谱法测定膨胀合金中硅.建立了硅的最佳测定条件,并在样品测定中对干扰因素进行了综合考虑.实验表明:该方法具有灵敏度高、选择性好,操作简便、容易掌握、分析周期短等优点.其相对标准偏差均小于1.0%(n=6).标准加入回收率均为97.0%~99.0%(n=6)范围内.可以作为检测膨胀合金中硅含量的一种手段.     

原子吸收光谱法测定镉镍电池浸渍液中硅

提出用一氧化二氮-乙炔火焰原子吸收光谱法测定镉镍电池浸渍液中硅含量。方法具有良好的灵敏度，干扰少，重现性好。硅量在5-50μg/mL范围内与吸光度呈良好的线性关系。其相对标准偏差均为1.0％；标准加入回收率在97.0％-103.0％范围内，适用于镉镍电池浸渍液中硅的分析。完全达到了实验室分析质量控制的要求。     

硅氢加成型室温固化硅橡胶胶粘剂的研究

<正> 我们研制了一种硅氢加成型室温固化硅橡胶,这种橡胶不但有较好的力学性能,而且与各类材料如金属、塑料、陶瓷、玻璃等都有很好的粘结力,是一种具有弹性的胶粘剂。该胶粘剂是利用一种含乙烯基聚硅氧烷、含氢聚硅氧烷以及二氧化硅补强剂在铂催化剂     

高性能陶瓷聚合物前驱体研究新进展

含硅聚合物是制备高性能陶瓷的重要前驱体。聚合物前驱体热解转化法在非氧化物陶瓷及其复合材料制备方面具有特别优势。本文主要介绍了含不饱和基团聚硅碳烷、线性和超支化聚硼硅氮烷、含过渡金属聚合物等几类前驱体的结构设计和合成新方法,以及其在电磁波吸收材料、锂电池负极材料、特种陶瓷结构3D打印成型方面应用的新进展。     

原子吸收法测定含锶卤水中的锂

研究了用空气-乙炔焰测定锂时,在火焰的不同高度处,共存盐类、酸类的干扰效应。对组成简单的试样,提供了可选用的火焰高度。观察到SrOH分子带对Li 6708埃线有严重的分子吸收。分析含锶卤水等试样时,建议加入磷酸钠,使喷雾测量液含pO_4~(3-)S2毫克/毫升,能有效地消除这种干扰;引入的Na~ 可作为电离阻止剂。     

一种火焰原子吸收分析的追加法

引言火焰原子吸收分析中最常采用的是校准曲线法。原子吸收分析的特点是干扰相对较少,所以容易配制绘制校准曲线用的校准溶液,有时使用只含待测元素的水溶液就能满足要求。但当遇有物理、化学、电离等干扰时,为消除干扰应使校准溶液的组成尽可能与试样溶液的组成一致。可是往往不易配制符合这一要求的校准溶液(尤其是分析试样的组成未知时),于是广泛采用着一种标准加入法。标准加入法须制备3～4份溶液,仍较繁琐,当试样量有限、分析元素的含量低     

Sc2MgGa2 and Y2MgGa2

Scandium magnesium gallide, Sc₂MgGa₂, and yttrium magnesium gallide, Y₂MgGa₂, were synthesized from the corresponding elements by heating under an argon atmosphere in an induction furnace. These intermetallic compounds crystallize in the tetragonal Mo₂FeB₂‐type structure. All three crystallographically unique atoms occupy special positions and the site symmetries of (Sc/Y, Ga) and Mg are m2m and 4/m, respectively. The coordinations around Sc/Y, Mg and Ga are pentagonal (Sc/Y), tetragonal (Mg) and triangular (Ga) prisms, with four (Mg) or three (Ga) additional capping atoms leading to the coordination numbers [10], [8+4] and [6+3], respectively. The crystal structure of Sc₂MgGa₂ was determined from single‐crystal diffraction intensities and the isostructural Y₂MgGa₂ was identified from powder diffraction data.     

Electrochemical study of (NEt4)2Cl2FeS2MoS2 and (NEt4)2Cl2FeS2MoS2FeCl2

Summary The ability of [MoS₄]^2–, anions to be used as ligands for transition metal ions has been widely demonstrated, especially with Fe²⁺. The present study has been restricted to linear complexes such as (NEt₄)₂ [Cl₂FeS₂MoS₂] and (NEt₄)₂[Cl₂FeS₂MoS₂FeCl₂]. Their electrochemical properties are described: upon electrochemical reduction, these compounds yield MoS₂, as a black precipitate, and an iron complex in solution, assumed to be [SFeCl₂]^2–. The electrochemical reduction goes through two electron transfers, coupled with the breakdown of the molecular skeleton: a DISPl and an ECE mechanism. Depending on the solvent, the following equilibrium may be observed: [Cl₄Fe₂MoS₄]^2–[Cl₂FeMoS₄]^2–+FeCl₂. The equilibrium constant, K_D, was evaluated by differential pulse polarography. K_D is tightly related to the donor number of the solvent.     

The alkali hypophosphites KH2PO2, RbH2PO2 and CsH2PO2

The structures of the hypophosphites KH₂PO₂ (potassium hypophosphite), RbH₂PO₂ (rubidium hypophosphite) and CsH₂PO₂ (caesium hypophosphite) have been determined by single‐crystal X‐ray diffraction. The structures consist of layers of alkali cations and hypophosphite anions, with the latter bridging four cations within the same layer. The Rb and Cs hypophosphites are isomorphous.     

Zur Kenntnis der Dialkalimetalldichalkogenide β-Na2S2, K2S2, α-Rb2S2, β-Rb2S2, K2Se2, Rb2Se2, α-K2Te2, β-K2Te2 und Rb2Te2

On Dialkali Metal Dichalcogenides β-Na₂S₂, K₂S₂, α-Rb₂S₂, β-Rb₂S₂, K₂Se₂, Rb₂Se₂, α-K₂Te₂, β-K₂Te₂ and Rb₂Te₂ The first presentation of pure samples of α- and β-Rb₂S₂, α- and β-K₂Te₂, and Rb₂Te₂ is described. Using single crystals of K₂S₂ and K₂Se₂, received by ammonothermal synthesis, the structure of the Na₂O₂ type and by using single crystals of β-Na₂S₂ and β-K₂Te₂ the Li₂O₂ type structure will be refined. By combined investigations with temperature-dependent Guinier-, neutron diffraction-, thermal analysis, and Raman-spectroscopy the nature of the monotropic phase transition from the Na₂O₂ type to the Li₂O₂ type will be explained by means of the examples α-/β-Na₂S₂ and α-/β-K₂Te₂. A further case of dimorphic condition as well as the monotropic phase transition of α- and β-Rb₂S₂ is presented. The existing areas of the structure fields of the dialkali metal dichalcogenides are limited by the model of the polar covalence.     

Formal [(2+2)+2] and [(2+2)+(2+2)] nonconjugated dienediyne cascade cycloadditions

[reaction: see text] Fluoranthene 2 and heptacycle 3 are easily accessible from the reaction of diyne 1 and norbornadiene (NBD) in the presence of the rhodium catalyst. The unusual [(2+2)+(2+2)] adduct 3 was confirmed by the X-ray crystal structure analysis.     

Crystal Structures of [Bu2Sn(O2PPh2)2], [Ph2Sn(O2PPh2)2], and [PhClSn(O2PPh2)OMe]2. Raman Spectra of [Ph2Sn(O2PPh2)2] and [PhClSn(O2PPh2)OMe]2

[(n‐Bu)₂Sn(O₂PPh₂)₂] ( 1 ), and [Ph₂Sn(O₂PPh₂)₂] ( 2 ) have been synthesized by the reactions of R₂SnCl₂ (R=n‐Bu, Ph) with HO₂PPh₂ in Methanol. From the reaction of Ph₂SnCl₂ with diphenylphosphinic acid a third product [PhClSn(O₂PPh₂)OMe]₂ ( 3 ) could be isolated. X‐ray diffraction studies show 1 to crystallize in the monoclinic space group P2₁/c with a = 1303.7(1) pm, b = 2286.9(2) pm, c = 1063.1(1) pm, β = 94.383(6)°, and Z = 4. 2 crystallizes triclinic in the space group , the cell parameters being a = 1293.2(2) pm, b = 1478.5(4) pm, c = 1507.2(3) pm, α = 98.86(3)°, β = 109.63(2)°, γ = 114.88(2)°, and Z = 2. Both compounds form arrays of eight‐membered rings (SnOPO)₂ linked at the tin atoms to form chains of infinite length. The dimer 3 consists of a like ring, in which the tin atoms are bridged by methoxo groups. It crystallizes triclinic in space group with a = 946.4(1) pm, b = 963.7(1) pm, c = 1174.2(1) pm, α = 82.495(6)°, β = 66.451(6)°, γ = 74.922(6)°, and Z = 1 for the dimer. The Raman spectra of 2 and 3 are given and discussed.     

Die Photoionenspektren von SCl2, S2Cl2 und S2Br2

Photoionization Mass Spectra of SCl₂, S₂Cl₂, and S₂Br₂ Photoionization mass spectra of SCl₂, S₂Cl₂, and S₂Br₂ have been measured. Heats of formation, bond energies, and ionization potentials of fragments have been calculated from appearance potentials.