Mg2NiQ6（Q=H，D，T）体系的热力学氢同位素效应

为研究Mg2NiQ4(Q=H,D,T)体系的热力学氢同位素效应,基于量子力学第一原理,采用密度泛函与赝势平面波相结合的方法,计算了Mg2NiQ6(Q=H,D,T)体系的声子色散谱,利用声子色散谱得到了热力学函数.利用文献报道的氢同位素气体分子的热力学数据,采用热力学方法分析了Mg2Ni吸氢形成Mg2NiQ6的同位素效应.研究结果表明,Mg2Ni吸氢的同位素效应主要是原子相对振动的频率不同导致的.CaF2结构的Mg2NiQ6的氢同位素效应随温度升高由负同位素效应转变为正同位素效应.     

氢化燃烧法合成La2-xNixMg17(x=0.5,1,1.5)材料的储氢性能

采用氢化燃烧法制备La2-xNixMg17(x=0.5, 1, 1.5)三元体系储氢材料, 对其热力学、动力学进行研究发现: 该体系材料具有很好的活性和较高的储氢量, 其中La1.5Ni0.5Mg17在573 K时吸放氢量分别为5.40和5.15 mass% H. 在553 K下, 体系α-β相区在600 s之内吸放氢反应分数均大于91%, 随着含Ni量的增加材料储氢容量降低, 吸放氢速率增大.物相分析知道体系吸氢后的主相是MgH2, 放氢后主相为Mg, 同时存在Mg2Ni, LaNi5或LaH3等催化物质, 从而使材料的氢化动力学性能得以明显改善.     

Mg-20%(RE-Ni)(RE=La,Y,Mm)复合材料储放氢性能研究

通过磁悬浮熔炼和反应球磨相结合的方法成功制备出Mg-20wt%(RE-Ni)(RE=La,Y,Mm)复合储氢材料,主要研究了材料的物相结构和储放氢性能.结果表明.Mg-20wt%(RE-Ni)(RE=La,Y,Mm)复合储氢材料,具有相似的物相结构和吸放氢热力学性能,吸氢相均为MgH2和Mg2Ni,在同一温度下,合金只有一个放氢平台,表明两相具有良好的协同放氢效应.在复合体系中,Mg-20wt%(Y-Ni)具有最佳的综合储氢性能,表明Y具有最佳的催化效果,其在293 K,3.0 MPa H2,10 min的吸氢量和573 K,对0.1 MPa,15 min的放氢量可分别达到3.92%和4.75%,实现了室温快速大量吸氢和较温和条件下的快速放氢.     

La-H化合物对LaMg2Ni合金中Mg2Ni相吸氢过程的影响

采用感应熔炼技术在Ar气氛保护下制备得到LaMg2Ni与Mg2Ni合金。X射线衍射(XRD)图表明LaMg2Ni合金在吸氢过程中分解为LaH3相和Mg2NiH4相,放氢过程中LaH3相转化为La3H7相。与Mg2Ni合金相比,LaMg2Ni合金显示出优良的吸氢动力学性能,这是由于镧氢化合物的存在及其在吸氢过程中所发生的相转变所造成的。LaMg2Ni合金280 s内吸氢即可达到最大储氢量的90%以上,而Mg2Ni合金则需要1200 s才能达到,且在相同温度下LaMg2Ni合金的吸氢反应速率常数大于Mg2Ni合金速率常数。镧氢化合物不仅有利于改善动力学性能,而且可以提高热力学性能。LaMg2Ni合金中的Mg2Ni相氢化反应焓与熵分别为-53.02 kJ.mol-1和84.96 J.K-1.mol-1(H2),这一数值小于单相Mg2Ni氢化反应焓与熵(-64.50 kJ.mol-1,-123.10 J.K-1.mol-1(H2))。压力-组成-温度(P-C-T)测试结果表明在603 K至523 K温度范围内,LaMg2Ni合金储氢容量保持稳定为1.95wt%左右,然而Mg2Ni合金的储氢容量则由4.09wt%衰减为3.13wt%,Mg2Ni合金的储氢容量在523K低温下仅为603 K时的76.5%,表明镧氢化合物能够改善Mg2Ni合金低温下的吸放氢性能。     

氢同位素双原子分子的解析势能函数

研究从重水中分离出T2 .首先,根据光谱常数导出氢同位素双原子分子Extended Rydberg的分析函数,基于同位素效应计算OT(X 2Пi)的光谱常数,有助导出三原子分子,如DTO 的解析势能函数.将这些Extended Rydberg解析势能函数用于氘交换分离氚的热力学与分子反应动力学研究.此外,由同位素位移极值得到当振动量子数vmax≈11.5,振动能级间隔△Ev(H2)≈△Ev(T2),若v△Ev(T2)和v>vmax时,△Ev(H2)<△Ev(T2).因而,温度较低时,平衡移向T2;温度较高时,平衡移向H2 .与文献结果相似 ,而导出方法不同.     

根据计算结构因子重新指定镍(II)8-羟基喹啉的两个络合物

晶体学研究曾认为,分子式是Na[NiQ2(HQ)](CLO4)的结构并不含有钠而应为[H3O][NiQ2(HQ)](CLO4).相似地,稀土－Ni络合物[YQ(HQ)2][NiQ3](CLO4)也不含有钇而应为[H3O][Ni2Q3(HQ)3](CLO4).晶体结构描述的修正系根据文献报导的原子坐标计算结构因子所导出的结果.     

镁基非晶电极合金充放氢过程中的组织结构演变及其热力学计算

采用熔体快淬法制备了(Mg70.6Ni29.4)90Nd10的非晶贮氢合金带,用X射线衍射仪和高分辨电镜对该合金在充放电循环过程中的组织结构演变进行了动态跟踪。结果表明:非晶(Mg70.6Ni29.4)90Nd10贮氢合金在充放电循环过程中经过4个循环以后开始晶化,首先生成平均颗粒尺寸为5 nm左右的NdMg2Ni9相,经过6个循环以后开始出现Mg2Ni相,到第20个循环后,生成了稳定的Mg2Ni,α-Mg和Nd2H5相。这表明初生相NdMg2Ni9在充放电循环过程中逐渐转化为Mg2Ni,α-Mg和Nd2H5相。经过热力学计算进一步验证表明,非晶(Mg70.6Ni29.4)90Nd10合金在晶化过程中首先形成NdMg2Ni9相,因为它的自由能(ΔG=-15.2789 kJ.mol-1,T=300 K)与Mg-Ni相(ΔG=-8.2694 kJ.mol-1,T=300 K)和Mg-Nd相(ΔG=-13.29503 kJ.mol-1,T=300 K)相比是最低的。     

Mg_2Ni_(1-x)Co_x合金相的固溶烧结法制备及结构和储氢性能

采用固溶烧结法制备了Mg_2Ni_(1-x)Co_x(x=0.10,0.15,0.20)合金,利用X射线衍射仪和压力-组成-温度测试仪等研究了Co含量对合金相结构和储氢性能的影响.结果表明,合金由Mg_2Ni型Mg_2(Ni,Co)主相及少量Mg和Mg Ni3Co新相组成.Mg2(Ni,Co)具有良好的可逆储氢性能,吸氢形成Mg_2Ni_(0.9)Co_(0.1)H_4型四元氢化物,其具有与父系氢化物HT-Mg_2NiH_4相近的放氢焓变(ΔHd=63.9 k J/mol H2).Mg_2Ni_(1-x)Co_x(x=0.10,0.15,0.20)合金具有良好的放氢动力学性能,二维相界面迁移为放氢过程的控制步骤.随着Co含量的增加,合金的放氢活化能(Ea)降低,其中,Mg_2Ni_(0.8)Co_(0.2)的Ea降低到54.0 k J/mol.     

Pd取代对Mg2Ni及其氢化物结构和性能影响的第一性原理研究

利用基于第一性原理的密度泛函理论,计算了镁基储氢合金Mg2 Ni以及Pd取代的合金Mg12 Ni6-xPdx(x1,2,3)及其氢化物H2-Mg12 Ni6-xPdx(x=0,1,2,3)的晶体结构和电子结构.结果表明,Pd取代Mg2 Ni中的Ni原子,使其晶胞体积有所膨胀.同时,Pd的取代对Mg-Ni和Ni-Ni间的...     

锆氢化反应热力学函数的计算

用B3LYP/SDD密度泛函方法计算了ZrH的微观性质,气态ZrH(D,T)的能量(E),熵(S)以及 Zr与氢同位素气体反应的热力学函数.在ZrH(s)、ZrD(s)和ZrT(s)的E和S的计算中,近似以分 子总能量中的振动能Ev代替固态能量,以电子和振动熵SEv代替固态熵.在这种近似下,计算了 不同温度下Zr与H2、D2、T2反应的ΔH、ΔG、ΔS及氢化反应平衡压力,导出了与温度 的依赖关系.计算结果表明,ZrH(s)的生成热为161.34 kJ穖ol-1,与实验值(173.5 kJ穖ol -1)接近,表明这种近似处理方法是合理的,可以用于研究贮氢材料氢化反应的热力学.     

Thermochemistry and accurate quantum reaction rate calculations for H2/HD/D2 + CH3

Accurate quantum-mechanical results for thermodynamic data, cumulative reaction probabilities (for J = 0), thermal rate constants, and kinetic isotope effects for the three isotopic reactions H2 + CH3 --> CH4 + H, HD + CH3 --> CH4 + D, and D2 + CH3 --> CH(3)D + D are presented. The calculations are performed using flux correlation functions and the multiconfigurational time-dependent Hartree (MCTDH) method to propagate wave packets employing a Shephard interpolated potential energy surface based on high-level ab initio calculations. The calculated exothermicity for the H2 + CH3 --> CH4 + H reaction agrees to within 0.2 kcal/mol with experimentally deduced values. For the H2 + CH3 --> CH4 + H and D2 + CH3 --> CH(3)D + D reactions, experimental rate constants from several groups are available. In comparing to these, we typically find agreement to within a factor of 2 or better. The kinetic isotope effect for the rate of the H2 + CH3 --> CH4 + H reaction compared to those for the HD + CH3 --> CH4 + D and D2 + CH3 --> CH(3)D + D reactions agree with experimental results to within 25% for all data points. Transition state theory is found to predict the kinetic isotope effect accurately when the mass of the transferred atom is unchanged. On the other hand, if the mass of the transferred atom differs between the isotopic reactions, transition state theory fails in the low-temperature regime (T < 400 K), due to the neglect of the tunneling effect.     

Polarization IR spectra of hydrogen bonded pyrazole crystals: self-organization effects in proton and deuteron mixture systems. Long-range H/D isotopic effects

This paper deals with experimental studies of the polarization IR spectra of solid-state pyrazole H1345, as well as of its H1D345, D1H345 and D1345 deuterium derivatives. Spectra were measured for the vN-H and vN-D band frequency ranges at temperatures of 298 and 77 K. The spectra were found to strongly change their intensity distribution and their polarization properties with the decrease of temperature. These effects were ascribed to some temperature-induced conformational changes in the hydrogen bond lattices. The studies reported allowed the finding of new kind of isotopic effects H/D in the open-chain hydrogen bond systems, i.e. the self-organization effects. It was found that the spectrally active aggregates of hydrogen bonds remain unchanged despite the growing isotope H/D exchange rate. This statement was supported by analysis of the residual polarized vN-H and vN-D band properties, measured for the isotopically diluted crystalline samples. Analysis of the band shapes of the four hydrogen isotope derivative crystals proved the existence of another kind of H/D isotopic effect, i.e. the long-range isotopic effect. It depends on an influence of the pyrazole ring hydrogen atoms onto the vN-H and vN-D band widths and onto the band fine structures.     

Molecular hydrogen tweezers: structure and mechanisms by neutron diffraction, NMR, and deuterium labeling studies in solid and solution

The mechanism of reversible hydrogen activation by ansa-aminoboranes, 1-N-TMPH-CH(2)-2-[HB(C(6)F(5))(2)]C(6)H(4) (NHHB), was studied by neutron diffraction and thermogravimetric mass-spectroscopic experiments in the solid state as well as with NMR and FT-IR spectroscopy in solution. The structure of the ansa-ammonium borate NHHB was determined by neutron scattering, revealing a short N-H···H-B dihydrogen bond of 1.67 ?. Moreover, this intramolecular H-H distance was determined in solution to be also 1.6-1.8 ? by (1)H NMR spectroscopic T(1) relaxation and 1D NOE measurements. The X-ray B-H and N-H distances deviated from the neutron and the calculated values. The dynamic nature of the molecular tweezers in solution was additionally studied by multinuclear and variable-temperature NMR spectroscopy. We synthesized stable, individual isotopic isomers NDDB, NHDB, and NDHB. NMR measurements revealed a primary isotope effect in the chemical shift difference (p)Δ(1)H(D) = δ(NH) - δ(ND) (0.56 ppm), and hence supported dihydrogen bonding. The NMR studies gave strong evidence that the structure of NHHB in solution is similar to that in the solid state. This is corroborated by IR studies providing clear evidence for the dynamic nature of the intramolecular dihydrogen bonding at room temperature. Interestingly, no kinetic isotope effect was detected for the activation of deuterium hydride by the ansa-aminoborane NB. Theoretical calculations attribute this to an "early transition state". Moreover, 2D NOESY NMR measurements support fast intermolecular proton exchange in aprotic CD(2)Cl(2) and C(6)D(6).     

Spin-orbit relaxation of Cl(2P1/2) and F(2P1/2) in a gas of H2

The authors present quantum scattering calculations of rate coefficients for the spin-orbit relaxation of F(2P1/2) atoms in a gas of H2 molecules and Cl(2P1/2) atoms in a gas of H2 and D2 molecules. Their calculation of the thermally averaged rate coefficient for the electronic relaxation of chlorine in H2 agrees very well with an experimental measurement at room temperature. It is found that the spin-orbit relaxation of chlorine atoms in collisions with hydrogen molecules in the rotationally excited state j=2 is dominated by the near-resonant electronic-to-rotational energy transfer accompanied by rotational excitation of the molecules. The rate of the spin-orbit relaxation in collisions with D2 molecules increases to a great extent with the rotational excitation of the molecules. They have found that the H2/D2 isotope effect in the relaxation of Cl(2P1/2) is very sensitive to temperature due to the significant role of molecular rotations in the nonadiabatic transitions. Their calculation yields a rate ratio of 10 for the electronic relaxation in H2 and D2 at room temperature, in qualitative agreement with the experimental measurement of the isotope ratio of about 5. The isotope effect becomes less significant at higher temperatures.     

Isotope effects on the unimolecular dissociation of ionized 3-methyl-2-butanol: reactions via a long-lived C-H-C hydrogen-bridged ion-neutral complex

A pronounced isotope effect causes metastable CD3CHOHCH(CH3)2+* ions to expell C3H6D2 in preference to C3H7D in a ratio of approximately 33:1; a number of related compounds show similar effects. High-level ab initio calculations suggest that the reactant alcohol molecular ion possesses an extraordinarily long alpha-carbon-carbon bond and that the reaction proceeds via the formation of an intermediate hydrogen-bridged complex of propane and ionized vinyl alcohol, in which the bridging hydrogen atom is almost midway between the two carbon termini. The isotopic preference reflects the difference between the zero-point vibrational energies of the isotopically different product pairs rather than kinetic isotope effects on the hydrogen atom transfer reactions that precede dissociation.     

Stabilization of the previously unknown tautomer HP(OH)2 of hypophosphorous acid as ligand; preparation of [W3(Ni(HP(OH)2))Q4(H2O)9]4+ (Q = S,Se) complexes

Bis(hydroxy)phosphine, the isomer of hypophosphorous acid which remained elusive for a long time, coordinates to the Ni site of heterometallic clusters with a W3NiQ4 core (Q = S, Se) to give [W3(Ni(HP(OH)2))Q4(H2O)9]4+ (Q = S, Se).     

Temperature dependence of fractionation of hydrogen isotopes in aqueous sodium chloride solutions

The D/H ratios of hydrogen gas in equilibrium with aqueous sodium chloride solutions of 2, 4 and 6 molalities were determined within the range 10 to 95°C, using a hydrophobic platinum catalyst. With each of the different sodium chloride concentrations, the hydrogen isotope effect between the solution and pure water changes linearly with the square of the reciprocal temperature. On the basis of the results for hydrogen isotope fractionation observed in this study, and those of hydrogen isotope fractionation between pure water and vapor, it is concluded that the structure of the aqueous sodium chloride solution does not change significantly with temperature. The hydrogen isotope effect is evidently different from the results of vapor pressure isotope effects (VPIE) on sodium chloride solutions measured on separated isotopes. The difference between the present work and the VPIE studies is probably due to a non-ideal behavior in a mixture of isotopic water molecules and/or to a H₂O-D₂O disproportionation reaction in sodium chloride solutions. The distinction between the latter two mechanisms can not be differentiated at present.     

氢键构筑的新颖微孔配位聚合物[Co2(Hisor)2·(4,4′-bpy)2(H2O)2]·4,4′-bpy的合成与结构

A novel microporous coordination polymer [Co2(Hisor)2(4,4′-bpy)2(H2O)2]·4,4′-bpy was synthesized by hydrothermal reaction and characterized by single crystal X-ray diffraction, elemental analysis and IR spectrum. The crystal belongs to the monoclinic system and space group is P2/n with a=1.040 6(3) nm, b=1.138 8(4) nm, c=1.854 7(6) nm, β=102.991(6)°, V= 2.141 6(12) nm3, Z=2, Dc=1.443 Mg/m3, Mr=930.62, μ=0.842 mm-1, F(000)=952, GOF= 1.072, R=0.065 4, wR=0.146 8[I>2σ(I)]. There are two crystallographically independent Co(Ⅱ) ions in the title complex. The Hisor2- and 4,4′-bpy link the metal ions into 2D grids with dimension of 0.522 3 nm×1.138 8 nm. There are O—H…O and N—H…O hydrogen bonds in the complex resulting in the formation of 3D network with 1D channels, in which are free 4,4′-bpy molecules.     

Effect of pressure on a heavy-atom isotope effect of yeast alcohol dehydrogenase

Hydrostatic pressure causes a monophasic decrease in the (13)C primary isotope effect expressed on the oxidation of benzyl alcohol by yeast alcohol dehydrogenase. The primary isotope effect was measured by the competitive method, using whole-molecule mass spectrometry. The effect is, therefore, an expression of isotopic discrimination on the kinetic parameter V/K, which measures substrate capture. Moderate pressure increases capture by activating hydride transfer, the transition state of which must therefore have a smaller volume than the free alcohol plus the capturing form of enzyme [Cho, Y.-K.; Northrop, D. B. Biochemistry 1999, 38, 7470-7475]. The decrease in the (13)C isotope effect with increasing pressure means that the transition state for hydride transfer from the heavy atom must have an even smaller volume, measured here to be 13 mL.mol(-1). The pressure data factor the kinetic isotope effect into a semiclassical reactant-state component, with a null value of k(12)/k(13) = 1, and a transition-state component of Q(12)/Q(13) = 1.028 (borrowing Bell's nomenclature for hydrogen tunneling corrections). A similar experiment involving a deuterium isotope effect previously returned the same volume and null value, plus a pressure-sensitive isotope effect [Northrop, D. B.; Cho, Y.-K. Biochemistry 2000, 39, 2406-2412]. Consistent with precedence in the chemical literature, the latter suggested a possibility of hydrogen tunneling; however, it is unlikely that carbon can engage in significant tunneling at ambient temperature. The fact that the decrease in activation volumes for hydride transfer is equivalent when one mass unit is added to the carbon end of a scissile C-H bond and when one mass unit is added to the hydrogen end is significant and suggests a common origin.