三元配合物RE(Et2dtc)3(phen)热化学性质的规律性

在无水乙醇中, 用铜试剂(NaEt₂dtc•3H₂O)和邻菲咯啉(o-phen•H₂O)分别与13种低水合氯化稀土合成了三元固态配合物(其中5种尚未见文献报道), 确定它们的组成可用通式RE(Et₂dtc)₃(phen)表示. IR光谱表明配合物中RE³⁺与3个NaEt₂dtc中的6个硫原子双齿配位, 同时与o-phen中的2个氮原子双齿配位. 用RD496-Ⅲ微量热计测定了298.15 K下13种水合氯化稀土盐及两个配体在无水乙醇中的溶解焓, 两个配体醇溶液的混合焓及13种化合物液相生成反应的焓变, 并通过合理的热化学循环, 求得了标题配合物的固相生成反应焓变; 测定了标题配合物298.15 K的比热容. 用RBC-II精密转动弹热量计测定了标题配合物的恒容燃烧热, 计算了它们的标准摩尔燃烧焓和标准摩尔生成焓. 发现系列配合物RE(Et₂dtc)₃(phen) (RE＝La, Pr, Nd, Sm～Lu)的多项热化学性质, 如低水合氯化稀土盐在无水乙醇中的溶解焓以及配合物的液相生成反应焓变和固相生成反应焓变、常温比热容、标准摩尔燃烧焓和标准摩尔生成焓都与稀土原子序数作图呈现“三分组现象”. 较集中地反映出配合物中RE³⁺与配体间的化学键有一定程度的共价性, 这是由于稀土离子5s²5p⁶轨道对4f电子的不完全屏蔽引起的.     

三元配合物RE(Et2dtc)3(phen)热化学性质的规律性

在无水乙醇中, 用铜试剂(NaEt₂dtc•3H₂O)和邻菲咯啉(o-phen•H₂O)分别与13种低水合氯化稀土合成了三元固态配合物(其中5种尚未见文献报道), 确定它们的组成可用通式RE(Et₂dtc)₃(phen)表示. IR光谱表明配合物中RE³⁺与3个NaEt₂dtc中的6个硫原子双齿配位, 同时与o-phen中的2个氮原子双齿配位. 用RD496-Ⅲ微量热计测定了298.15 K下13种水合氯化稀土盐及两个配体在无水乙醇中的溶解焓, 两个配体醇溶液的混合焓及13种化合物液相生成反应的焓变, 并通过合理的热化学循环, 求得了标题配合物的固相生成反应焓变; 测定了标题配合物298.15 K的比热容. 用RBC-II精密转动弹热量计测定了标题配合物的恒容燃烧热, 计算了它们的标准摩尔燃烧焓和标准摩尔生成焓. 发现系列配合物RE(Et₂dtc)₃(phen) (RE＝La, Pr, Nd, Sm～Lu)的多项热化学性质, 如低水合氯化稀土盐在无水乙醇中的溶解焓以及配合物的液相生成反应焓变和固相生成反应焓变、常温比热容、标准摩尔燃烧焓和标准摩尔生成焓都与稀土原子序数作图呈现“三分组现象”. 较集中地反映出配合物中RE³⁺与配体间的化学键有一定程度的共价性, 这是由于稀土离子5s²5p⁶轨道对4f电子的不完全屏蔽引起的.     

三元配合物Tm[(C_5H_8NS_2)_3(C_(12)H_8N_2)]的热化学性质研究

在无水乙醇中,用吡咯烷二硫代氨基甲酸铵(APDTC)和1,10-邻菲咯啉(o-phen·H2O)与TmCl3·3.65H2O作用,合成了未见文献报道的三元固态配合物,确定它的组成为Tm[(C5H8NS2)3(C12H8N2)]。用RD496-Ⅲ微量热计测定了298.15K下水合氯化铥及两个配体在无水乙醇中的溶解焓,两个配体醇溶液的混合焓及不同温度下标题化合物液相生成反应的焓变。在实验和计算基础上,得到了液相生成反应的热力学参数(活化焓、活化熵和活化自由能),速率常数和动力学参数(表现活化能、频率因子和反应级数)。通过合理的热化学循环,求得了298.15K时标题化合物的固相生成反应焓变;推导了用该热量计测定固态物质比热容的计算式,并测定了题目配合物298.15K的比热容。用RBC-Ⅱ精密转动弹热量计测定了题目配合物的恒容燃烧热,计算了它们的标准摩尔燃烧焓和标准摩尔生成焓。     

三元配合物Yb[(C5H8NS2)3(C12H8N2)]的热化学性质研究

在无水乙醇中, 用吡咯烷二硫代氨基甲酸铵(APDTC)和1, 10-邻菲咯啉(o-phen·H2O)与YbCl3·3.84H2O作用, 合成了三元固态配合物, 确定它的组成为Yb[(C5H8NS2)3(C12H8N2)]. 用RD496-Ⅲ微量热计测定了298.15 K下水合氯化镱及两个配体在无水乙醇中的溶解焓, 两个配体醇溶液的混合焓及不同温度下标题化合物液相生成反应的焓变; 得到了液相生成反应的热力学参数(活化焓、活化熵和活化自由能)和动力学参数(速率常数、表观活化能、频率因子和反应级数); 通过合理的热化学循环, 求得了298.15 K时标题化合物的固相生成反应焓变; 推导了用该热量计测定固态物质比热容的计算式, 并测定了该配合物298.15 K的比热容.     

离子液体C3MIBF4和C5MIBF4溶解焓的研究

在298.15 K下利用等温环境溶解反应热量计测定了离子液体C₃MIBF₄(四氟硼酸1-甲基-3-丙基咪唑)和C₅MIBF₄(四氟硼酸1-甲基-3-戊基咪唑)不同浓度水溶液的摩尔溶解焓(Δ_sH_m). 借助Pitzer电解质溶液理论, 得到了它们的标准摩尔溶解焓 和Pitzer焓参数: 和 , 并计算了表观相对摩尔焓. 根据Glasser理论计算了离子液体晶格能, 进而估算了离子液体C₅MIBF₄和C₃MIBF₄中正离子的水化焓分别为－171 kJ•mol^－1 (C₅MI^＋)和－207 kJ•mol^－1 (C₃MI^＋).     

乳酸配合物(NH4)2[Sr(C3H5O3)4]的晶体结构、Hirshfeld表面分析和溶液化学性质

合成了无水乳酸配合物(NH₄)₂[Sr(C₃H₅O₃)₄]。用X射线单晶衍射仪对该配合物的晶体结构进行了表征,确定了其组成、空间结构和配位方式。绘制了配合物的Hirshfeld表面和2D指纹图,揭示了分子间的相互作用以及该配合物具有多个配位位点和较强的配位活性。根据相关的晶体数据计算出了该配合物的晶格能及其对应阴离子的摩尔体积,计算得到该配合物的晶格能为2 742.9 kJ·mol^-1。用等温环境反应-溶解量热计测量了该配合物在298 K超纯水溶剂中的溶解焓。根据Pitzer电解质溶液理论,在298 K下获得了该配合物的无限稀释摩尔溶解焓Δ_sH_m^∞和Pitzer参数,确定该配合物的Δ_sH_m^∞为(114.01±0.04) kJ·mol^-1。计算了该配合物的表观相对摩尔焓(^ΦL)以及不同浓度下溶质和溶剂的相对偏摩尔焓(L₁和L₂)。最后,根据晶格能和Δ_sH_m^∞设计了热化学循环,并计算出了阴离子的水合焓值。热重和微商热重曲线进一步揭示了该配合物的结构。     

离子液体C3MIBF4和C5MIBF4溶解焓的研究

在298.15 K下利用等温环境溶解反应热量计测定了离子液体C₃MIBF₄(四氟硼酸1-甲基-3-丙基咪唑)和C₅MIBF₄(四氟硼酸1-甲基-3-戊基咪唑)不同浓度水溶液的摩尔溶解焓(Δ_sH_m). 借助Pitzer电解质溶液理论, 得到了它们的标准摩尔溶解焓 和Pitzer焓参数: 和 , 并计算了表观相对摩尔焓. 根据Glasser理论计算了离子液体晶格能, 进而估算了离子液体C₅MIBF₄和C₃MIBF₄中正离子的水化焓分别为－171 kJ•mol^－1 (C₅MI^＋)和－207 kJ•mol^－1 (C₃MI^＋).     

乳酸配合物(NH4)2[Sr(C3H5O3)4]的晶体结构、Hirshfeld表面分析和溶液化学性质

合成了无水乳酸配合物(NH₄)₂[Sr(C₃H₅O₃)₄]。用X射线单晶衍射仪对该配合物的晶体结构进行了表征,确定了其组成、空间结构和配位方式。绘制了配合物的Hirshfeld表面和2D指纹图,揭示了分子间的相互作用以及该配合物具有多个配位位点和较强的配位活性。根据相关的晶体数据计算出了该配合物的晶格能及其对应阴离子的摩尔体积,计算得到该配合物的晶格能为2742.9 kJ·mol^-1。用等温环境反应-溶解量热计测量了该配合物在298 K超纯水溶剂中的溶解焓。根据Pitzer电解质溶液理论,在298 K下获得了该配合物的无限稀释摩尔溶解焓△_sH_m^∞和Pitzer参数,确定该配合物的△_sH_m^∞为(114.01±0.04) kJ·mol^-1。计算了该配合物的表观相对摩尔焓(^ΦL)以及不同浓度下溶质和溶剂的相对偏摩尔焓(L₁和L₂)。最后,根据晶格能和△_sH_m^∞设计了热化学循环,并计算出了阴离子的水合焓值。热重和微商热重曲线进一步揭示了该配合物的结构。     

稀土配合物[Pr(C3H7NO2)2(C3H4N2)(H2O)](ClO4)3的标准生成焓及热分解动力学研究

合成了高氯酸镨和咪唑(C₃H₄N₂), DL-α-丙氨酸(C₃H₇NO₂)混配配合物晶体. 经傅立叶变换红外光谱、化学分析和元素分析确定其组成为[Pr(C₃H₇NO₂)₂(C₃H₄N₂)(H₂O)](ClO₄)₃. 使用具有恒温环境的溶解-反应量热计, 以2.0 mol•L^－1 HCl为量热溶剂, 在T＝(298.150±0.001) K时测定出化学反应PrCl₃•6H₂O(s)＋2C₃H₇NO₂(s)＋C₃H₄N₂(s)＋3NaClO₄(s)＝[Pr(C₃H₇NO₂)₂(C₃H₄N₂)(H₂O)](ClO₄)₃(s)＋3NaCl(s)＋5H₂O(1)的标准摩尔反应焓为Δ_rH_m^ө＝(39.26±0.11) kJ•mol^－1. 根据盖斯定律, 计算出配合物的标准摩尔生成焓为Δ_fH_m^ө{[Pr(C₃H₇NO₂)₂(C₃H₄N₂)(H₂O)](ClO₄)₃(s), 298.150 K}＝(－2424.2±3.3) kJ•mol^－1. 采用TG-DTG技术研究了配合物在流动高纯氮气(99.99%)气氛中的非等温热分解动力学, 运用微分法(Achar-Brindley-sharp和Kissinger法)和积分法(Satava-Sestak和Coats-Redfern法)对非等温动力学数据进行分析, 求得分解反应的表观活化能E＝108.9 kJ•mol^－1, 动力学方程式为dα/dt＝2(5.90×10⁸/3)(1－α)[－ln(1－α)]^－1exp(－108.9×10³/RT).     

RE(C5H8NS2)3(C12H8N2)的标准摩尔生成焓

在无水乙醇中, 使低水合氯化稀土 (RE = Ho, Er, Tm, Yb, Lu) 与吡咯烷二硫代氨基甲酸铵 (APDC)和1,10-菲咯啉 (o–phen•H₂O) 反应, 制得其三元固态配合物. 用化学分析和元素分析确定它的组成为RE(C₅H₈NS₂)₃(C₁₂H₈N₂) (RE = Ho, Er, Tm, Yb, Lu). IR光谱说明RE³⁺ 分别与3个PDC^–的6个硫原子双齿配位, 同时与o–phen的2个氮原子双齿配位, 配位数为8. 用精密转动弹热量计测定了它们的恒容燃烧热△_cU分别为(-16788.46 ± 7.74), (-15434.53 ± 8.28), (-15287.80 ± 7.31), (-15200.50 ± 7.22)和(-15254.34 ± 6.61) kJ•mol^-1; 并计算了它们的标准摩尔燃烧焓△_cH_m^θ和标准摩尔生成焓△_fH_m^θ分别为( -16803.95 ± 7.74), (-15450.02 ± 8.28), (-15303.29 ± 9.28), (-15215.99 ± 7.22), (-15269.83 ± 6.61) kJ • mol^-1和 (-1115.42 ± 8.94), (-2477.80 ± 9.15), (-2619.95 ± 10.44), (-2670.17 ± 8.22), (-2650.06 ± 8.49) kJ•mol^-1.     

Vapour-liquid equilibrium data for the systems C2H6 + N2, C2H4 + N2, C3H8 + N2, and C3H6 + N2

High pressure vapour-liquid equilibrium data for the C₂H₆ + N₂, C₂H₄ + N₂, C₃H₈ + N₂, and C₃H₆ + N₂ systems are presented. The data are obtained isothermally in the range from 200 K to 290 K. For each point of data, temperature, pressure and liquid and vapour phase mole fractions are measured.Values for the vapour phase mole fractions are calculated from the obtained pressure, temperature and liquid phase mole fractions. The calculated values are compared with the experimental results, and it is found that the average mean deviation between calculated and experimental mole fractions is less than 0.009 for the systems considered in this work.     

Die Trennung von Ar und O2 sowie CH4, C2H6, C3H8 und C4H10

Ohne Zusammenfassung     

Synthesis and crystal structures of (C8h8)Nd(C5H9C5H4) (THF)2 and [(C8H8)Gd(C5H9C4H4(THF)][(C8H8)GD(C5H9C5H4(THF)2]

LnCl₃ (Ln=Nd, Gd) reacts with C₅H₉C₅H₄Na (or K₂C₈H₈) in THF (C₅H₉C₅H₄ = cyclopentylcyclopentadienyl) in the ratio of 1 : to give (C₅H₉C₅H₄)LnCl₂(THF)_n (orC₈H₈)LnCl₂(THF)_n], which further reacts with K₂C₈H₈ (or C₅H₉C₅H₄Na) in THF to form the litle complexes. If Ln=Nd the complex (C₈H₈)Nd(C₅H₉C₅H₄)(THF)₂ (a) was obtained: when Ln=Gd the 1 : 1 complex [(C₈H₈)Gd(C_%H₉)(THF)][(C₈H₈)Gd(C₅H₉H₄)(THF)₂] (b) was obtained in crystalline form.

The crystal structure analysis shows that in (C₈H₈)Ln(C₅H₉C₅H₄)(THF)₂ (Ln=Nd or Gd), the Cyclopentylcyclopentadieny (η⁵), cyclooctatetraenyl (η⁸) and two oxygen atoms from THF are coordinated to Nd³⁺ (or Gd³⁺) with coordination number 10.

The centroid of the cyclopentadienyl ring (Cp′) in C₅H₉C₅H₄ group, cyclooctatetraenyl centroid (COTL) and two oxygens (THF) form a twisted tetrahedron around Nd³⁺ (or Gd³⁺). In (C₈H₈)Gd(C₅H₉C₅H₄)(THF), the cyclopentyl-cyclopentadienyl (η⁵), cyclooctatetraenyl (η⁸) and one oxygen atom are coordinated to Gd³⁺ with the coordination number of 9 and Cp′, COT and oxygen atom form a triangular plane around Gd³⁺, which is almost in the plane (dev. -0.0144 Å).     

Multiconfiguration self-consistent wavefunctions for CH4, C2H4 and C2H6

The results of several MC SCF calculations on CH₄, C₂H₄ and C₂H₆ with minimun bases of Slater type AO's are reported. The computing method is a quadratically convergent process. Better final energies are obtained if localized MO's are used.     

Surface-enhanced raman spectra of C2H2 and C2H4 adsorbed on silver colloid

We report the surface-enhanced Raman spectra of ethylene and acetylene adsorbed on colloidal silver particles formed by gas aggregation and isolated at low temperatures in solid adsorbate/argon matrices. The spectra of both molecules exhibit modes which are normally Raman-forbidden. Excitation with several visible laser frequencies indicated that the degree of enhancement increased towards the blue.     

Reactions of the dications C7H6, C7H7, and C7H8 with methane: Predominance of doubly charged intermediates

The reactions of methane with the dications C₇H₆²⁺, C₇H₇²⁺, and C₇H₈²⁺ generated by electron ionization of toluene are studied using mass-spectrometry tools. It is shown that the reactivity is dominated by the formation of doubly charged intermediates, which can either eliminate molecular hydrogen to yield doubly charged products or undergo charge-separation reactions leading to the formation of a methyl cation and the corresponding C₇H_n+1⁺ monocation. Typical processes observed for dications, like electron transfer or proton transfer, are largely suppressed. The theoretically derived mechanism of the reaction between C₇H₆²⁺ and CH₄ indicates that the formation of the doubly charged intermediate is kinetically preferred at low internal energies of the reactants. In agreement, the experimental results show a pronounced hydrogen scrambling and dominant formation of the doubly charged products at low collision energies, whereas direct hydride transfer prevails at larger collision energies.     

Kinetic isotope effects in the reaction H + C2H4 → C2H5

The high-pressure limiting rate constants of the reactions between H or D atoms and three isotopic ethylenes have been measured in the temperature range 206–461 K. Practically no isotope effects due to the differences between the ethylenes could be observed. This result does not agree with the prediction recently made by the activated complex theory.     

Electron scattering differential cross sections for C2H2, C2H4, and C2H6 by gas phase electron diffraction - binding effects

Experimental differential cross sections for 40 keV electrons scattered by C₂H₂, C₂H₄ and C₂H₆ molecules were measured using the gas electron diffraction method in the range of the scattering variable s from s = 1 A^?1 to s = 30 A^?1. The differential cross sections for neon were also measured and compared with calculated differential cross sections to calibrate the diffractograph. Experimental differential cross sections show significant deviations with respect to theoretical differential cross sections calculated from the Debye-Ehrenfest model, mainly in the range of small scattering angles. The observed differences are connected to chemical binding effects. From the experimental data, an estimation of the binding energy was carried out. The deduced values: ?0.58 ± 0.20 au for C₂H₂, ?0.94 ± 0.30 au for C₂H₄ and ?1.23 ± 0.40 au for C₂H₆ are in agreement with those obtained by thermochemical methods.     

Reactions of C2(a 3πu) with CH4, C2H2, C2H4, C2H6, and O2 using multiphoton UV excimer laser photolysis

C₂(a ³π_u) disappearance rate constants of 1.44, 0.96, 0.0296, 0.0130 and < 10^?6(x10^?10cm³s^?1) are reported for reactions with C₂H₄, C₂H₂, O₂, C₂H₆, and CH₄, respectively at 298 K. C₂(a ³π_u) fragments are generated by multiphoton ArF excimer laser photodissociation at C₂H₂, and monitored by dye laser induced fluorescence. Arguments are presented which favor chemical reactions over the C₂(a ³π_u) → (X ¹σ⁺_g) quenching channel. C₂ + C₂H₂ represents the one possible exception to the reactive channel.     

Evidence for the distortion of C2H4 and C2H2 chemisorbed on W(100)

The adsorption of C₂H₄ on W(100) has been studied by ultraviolet photoelectron spectroscopy with hν = 21.22 eV. The spectrum measured after in initial saturation exposure at 80 K exhibits structure which correlates well with energy levels recently calculated by Demuth and Eastman (DE) for sp³ rehybridized C₂H₄. Dehydrogenation of the adsorbate, either by subsequent heating to 295 K or direct adsorption at 295 K, yields a spectrum which correlates with DE's calculation for sp² rehybridized C₂H₂. These results suggest that C₂H₄ and C₂H₂ may be distorted from their planar and linear structures respectively and that the CC bonds on these molecules are stretched by adsorption on W(100). Qualitative arguments suggest that the bonding site for both melecules is directly over a W atom and that the Dewar—Chatt model for πd bonding in organometallic compounds is applicable.