新型的含硫族元素碳硼烷配体的三(3，5-二甲基-1-吡唑)硼氢钼配合物的合成和分子结构(英)

三齿单核三(3，5-二甲基-1-吡唑)硼氢钼配合物Tp^*Mo(O)Cl₂ (1)(Tp^*=三(3，5-二甲基-1-吡唑)硼氢HB(C₃H(Me₂)N₂)₃)与含硫族元素碳硼烷的锂盐[(THF)₂LiE₂C₂B₁₀H₁₀(THF)]<     

磁性Co/TiB2室温高效催化氨硼烷产氢及串联降解有机污染物

通过熔盐法制备TiB₂载体,并采用简单的沉淀-沉积法制备了Co/TiB₂磁性可回收纳米催化剂,用于室温催化氨硼烷（NH₃BH₃）溶液产氢及串联降解对硝基苯酚（4-NP）及偶氮染料酸性橙7（AO7）、酸性红1（AR1）和甲基橙（MO）等有机污染物。采用X射线衍射、扫描电子显微镜、透射电子显微镜、X射线光电子能谱、振动样品磁强计等表征方法对催化剂的微观形貌和结构等进行分析。结果表明,Co纳米粒子均匀地分布在TiB₂载体表面,晶粒尺寸约为40 nm,并且被TiB₂载体包覆,具有典型的金属-载体强相互作用。Co/TiB₂表现出优异的室温催化NH₃BH₃溶液产氢活性,产氢速率为565.8 mol_H2·mol_cat^-1·h^-1。在串联降解有机污染物反应中,Co/TiB₂在7 min内催化4-NP氨基化的转化率接近100%,反应速率常数高达0.72 min^-1;降解AO7的反应速率常数在3种偶氮染料中最高（0.34 min^-1）。通过EPR-DMPO（EPR=电子顺磁共振,DMPO=5,5-二甲基-1-吡咯啉-N-氧化物）自由基捕获实验检测出Co/TiB₂+NH₃BH₃催化体系中产生大量的氢自由基（·H）。得益于·H的强还原性,Co/TiB₂+NH₃BH₃催化体系能够将4-NP氨基化为具有更高价值的对氨基苯酚（4-AP）,同时能够还原偶氮染料分子中的显色基团偶氮基（—N=N—）。     

LiMn(BH4)3/2LiCl复合物的反应球磨制备及其脱氢性能

以LiBH₄和MnCl₂为初始原料, 采用反应球磨法制备了LiMn(BH₄)₃/2LiCl复合物, 并系统地研究了该复合物的脱氢性能及含钛催化剂的掺杂对其脱氢性能的影响. 结果表明: LiMn(BH₄)₃/2LiCl复合物是由非晶态的LiMn(BH₄)₃和晶态的LiCl组成, 在135-190 °C分解, 分解反应的活化能为114.0 kJ·mol^-1; LiMn(BH₄)₃/2LiCl复合物分解失重约7.0% (w). 组分分析表明除H₂外, 释放的气体中还含有4.0% (摩尔分数, x)的B₂H₆. B₂H₆的生成是该复合物失重超过其理论储氢容量6.3% (w)的原因; 进一步研究发现, 含钛催化剂(TiF₃、TiC、TiN和TiO₂)中, 仅TiF₃能够催化LiMn(BH₄)₃/2LiCl复合物的分解反应, 使其起始分解温度和分解反应活化能分别降低至125 °C和104.0 kJ·mol^-1. 这主要归因于TiF₃中的Ti原子取代了LiMn(BH₄)₃中的部分Li原子, 并在局域形成了易于分解的Ti(BH₄)₃.     

N和F共掺杂C3N4的制备及其可见光催化性能

针对氮化碳（C₃N₄）光生电荷易复合、光催化性能有限的不足,我们制备N和F共掺杂C₃N₄（NF-C₃N₄）,以提升其光催化性能。利用NH₄F在高温下原位分解产生的HF和NH₃,对C₃N₄刻蚀的同时实现N和F双元素共掺杂。以氯化铵（NH₄Cl）为对照,制备N掺杂C₃N₄（N-C₃N₄）。利用扫描电子显微镜（SEM）、能谱仪（EDS）、X射线光电子能谱（XPS）、X射线衍射（XRD）、比表面积测试和电化学表征手段研究N、F共掺杂对C₃N₄形貌、成分、结构和物化性质等的影响规律。相比于C₃N₄和N-C₃N₄,NF-C₃N₄呈多孔状,比表面积增大,光生电荷的生成、分离和转移均被促进,NF-C₃N₄光催化还原Cr （Ⅵ）的速率是C₃N₄的2.6倍、N-C₃N₄的1.7倍。进一步考察了不同前驱体（尿素、双氰胺和三聚氰胺）对制备C₃N₄的影响,发现以尿素为前驱体的C₃N₄与NH₄F的质量比为3∶2时,NF-C₃N₄呈现最佳的光催化性能。催化剂用量、光照强度、空穴捕获剂浓度的增加和pH的降低均能提高Cr （Ⅵ）还原速率。在NF-C₃N₄浓度为0.1 g·L^-1、pH=3、c_EDTA-2Na=2 mmol·L^-1、40 min可见光照射后,Cr （Ⅵ）去除率达到90%。5次循环实验表明,优化制备的NF-C₃N₄光催化还原Cr （Ⅵ）的性能保持良好,具有较高的稳定性。     

Co/C3N4 NTs复合纳米材料的制备及光催化性能

采用化学还原法将非贵金属钴纳米颗粒沉积到氮化碳纳米管（C₃N₄ NTs）内外管壁,制备了Co/C₃N₄ NTs复合光催化剂。使用多种分析表征手段对Co/C₃N₄ NTs的形貌和结构进行分析,并比较Co负载量对复合材料可见光光催化产氢性能的影响。结果表明,该金属-半导体异质结可有效增强光生电子-空穴的分离速率。经可见光照射2 h后,当Co负载量为质量分数5%时具有最佳产氢量,且产氢速率为纯C₃N₄ NTs的1.7倍。     

RGO/C3N4复合材料的制备及可见光催化性能

通过半封闭一步热裂解法和改进的Hummers法分别制备了类石墨氮化碳(C₃N₄)和氧化石墨烯(GO),再利用光还原方法制得还原氧化石墨烯/氮化碳(RGO/C₃N₄)复合材料。采用X射线衍射(XRD),场发射扫描电镜(FESEM),X射线光电子能谱(XPS),紫外-可见漫反射吸收光谱(DRS),光致荧光(PL)和傅里叶变换红外光谱(FTIR)等测试技术对复合材料进行表征。以罗丹明B(RhB)为探针分子在可见光下考察RGO/C₃N₄复合材料的光催化活性,结果表明：RGO的引入显著提高了C₃N₄的光催化活性,且6.0%RGO/C₃N₄复合物的光催化活性最高,可能的原因是RGO具有优良的传导和接受电子性能,抑制了C₃N₄光生电子-空穴的复合机率,进而提高了光催化活性。     

四氯合锌酸正九烷铵的晶体结构及热化学性质

合成了四氯合锌酸正九烷铵复合物(C₉H₁₉NH₃)₂ZnCl₄(s) (C₉Zn(s)), 并使用X射线单晶衍射、化学分析以及元素分析确定了其晶体结构和化学组成. 利用其晶体学数据推导了C₉Zn(s)的晶格能U_POT=952.94 kJ·mol^-1. 在298.15 K下, 利用恒温环境溶解-反应热量计测定了C₉Zn(s)在不同质量摩尔浓度下的摩尔溶解焓. 在Pitzer电解质溶液理论基础上确定了C₉Zn(s)的无限稀释摩尔溶解焓Δ_sΗ_m^∞=20.09 kJ·mol^-1, 以及Pitzer焓参数组合(4β_C9H19NH3,Cl^(0)L+2β_Zn,Cl^(0)L+θ_C9H19NH3,Zn^L)和(2β_C9H19NH3,Cl^(1)L+β_Zn,Cl^(1)L)的值.     

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).     

全氟辛基磺酸稀土金属盐催化氟两相酯化反应

制备了全氟辛基磺酸稀土金属盐[RE(OSO₂C₈F₁₇)₃, RE＝Sc, Y, La～Lu]并研究了该催化剂作用下氟两相酯化反应. 全氟己烷(C₆F₁₄)、全氟甲苯(C₇F₈)、全氟甲基环己烷(C₇F₁₄)、全氟辛烷(C₈F₁₈)、1-溴代全氟辛烷(C₈F₁₇Br)和全氟萘烷(C₁₀F₁₈, 顺式与反式的混合物)可作为该反应的氟溶剂. 研究表明Yb(OSO₂C₈F₁₇)₃和C₁₀F₁₈分别是最好的氟代催化剂和氟溶剂. 以Yb(OSO₂C₈F₁₇)₃为催化剂在C₁₀F₁₈中苯甲酸和异戊醇的酯化反应得率为99%. 含有催化剂的氟相通过简单的相分离, 就可回收利用, 氟相重复使用5次, 其催化活性减少不大.     

溶液中肼还原钴离子制备纳米金属钴的反应动力学

通过加入NaBH₄作为诱导剂, 可在室温下引发肼与Co^2＋在水-乙醇体系中的还原反应, 制得高纯度纳米金属钴粉. 机理研究表明, 该反应分二段进行: 第一段主要发生Co^2＋被N₂H₄还原的反应(2Co^2＋＋N₂H₄＋4OH^－＝2Co¯＋N₂­＋4H₂O), 第二段主要为金属Co催化的肼分解反应(N₂H₄＝N₂­＋2H₂­)和歧化反应(3N₂H₄＝N₂­＋4NH₃­). Co^2＋被N₂H₄还原是典型的自催化过程, 因此, 加入少量NaBH₄即可在288 K下启动反应. 通过测量气体产物的生成速率, 获得了Co^2＋还原的反应动力学方程, 发现Co^2＋, N₂H₄和产物Co的反应级数分别为1, 0和1, 反应活化能约为89 kJ/mol. 调节Co^2＋的浓度, 纳米金属钴的表面积可从11增加到25 m²/g.     

Metal‐Borohydride‐Modified Zr(BH4)4⋅8 NH3: Low‐Temperature Dehydrogenation Yielding Highly Pure Hydrogen

Due to its high hydrogen density (14.8 wt %) and low dehydrogenation peak temperature (130 °C), Zr(BH₄)₄ ? 8 NH₃ is considered to be one of the most promising hydrogen‐storage materials. To further decrease its dehydrogenation temperature and suppress its ammonia release, a strategy of introducing LiBH₄ and Mg(BH₄)₂ was applied to this system. Zr(BH₄)₄ ? 8 NH₃–4 LiBH₄ and Zr(BH₄)₄ ? 8 NH₃–2 Mg(BH₄)₂ composites showed main dehydrogenation peaks centered at 81 and 106 °C as well as high hydrogen purities of 99.3 and 99.8 mol % H₂, respectively. Isothermal measurements showed that 6.6 wt % (within 60 min) and 5.5 wt % (within 360 min) of hydrogen were released at 100 °C from Zr(BH₄)₄ ? 8 NH₃–4 LiBH₄ and Zr(BH₄)₄ ? 8 NH₃–2 Mg(BH₄)₂, respectively. The lower dehydrogenation temperatures and improved hydrogen purities could be attributed to the formation of the diammoniate of diborane for Zr(BH₄)₄ ? 8 NH₃–4 LiBH₄, and the partial transfer of NH₃ groups from Zr(BH₄)₄ ? 8 NH₃ to Mg(BH₄)₂ for Zr(BH₄)₄ ? 8 NH₃–2 Mg(BH₄)₂, which result in balanced numbers of BH₄ and NH₃ groups and a more active H^δ+ ??? ^?δH interaction. These advanced dehydrogenation properties make these two composites promising candidates as hydrogen‐storage materials.     

A New Ammine Dual‐Cation (Li,Mg) Borohydride: Synthesis,Structure, and Dehydrogenation Enhancement

A new ammine dual‐cation borohydride, LiMg(BH₄)₃(NH₃)₂, has been successfully synthesized simply by ball‐milling of Mg(BH₄)₂ and LiBH₄ ? NH₃. Structure analysis of the synthesized LiMg(BH₄)₃(NH₃)₂ revealed that it crystallized in the space group P6₃ (no. 173) with lattice parameters of a=b=8.0002(1) Å, c=8.4276(1) Å, α=β=90°, and γ=120° at 50 °C. A three‐dimensional architecture is built up through corner‐connecting BH₄ units. Strong N? H???H? B dihydrogen bonds exist between the NH₃ and BH₄ units, enabling LiMg(BH₄)₃(NH₃)₂ to undergo dehydrogenation at a much lower temperature. Dehydrogenation studies have revealed that the LiMg(BH₄)₃(NH₃)₂/LiBH₄ composite is able to release over 8 wt % hydrogen below 200 °C, which is comparable to that released by Mg(BH₄)₃(NH₃)₂. More importantly, it was found that release of the byproduct NH₃ in this system can be completely suppressed by adjusting the ratio of Mg(BH₄)₂ and LiBH₄ ? NH₃. This chemical control route highlights a potential method for modifying the dehydrogenation properties of other ammine borohydride systems.     

Synergetic Effects of In Situ Formed CaH2 and LiBH4 on Hydrogen Storage Properties of the Li–Mg–N–H System

Hydrogen storage properties and mechanisms of the Ca(BH₄)₂‐doped Mg(NH₂)₂–2 LiH system are systematically investigated. It is found that a metathesis reaction between Ca(BH₄)₂ and LiH readily occurs to yield CaH₂ and LiBH₄ during ball milling. The Mg(NH₂)₂–2 LiH–0.1 Ca(BH₄)₂ composite exhibits optimal hydrogen storage properties as it can reversibly store more than 4.5 wt % of H₂ with an onset temperature of about 90 °C for dehydrogenation and 60 °C for rehydrogenation. Isothermal measurements show that approximately 4.0 wt % of H₂ is rapidly desorbed from the Mg(NH₂)₂–2 LiH–0.1 Ca(BH₄)₂ composite within 100 minutes at 140 °C, and rehydrogenation can be completed within 140 minutes at 105 °C and 100 bar H₂. In comparison with the pristine sample, the apparent activation energy and the reaction enthalpy change for dehydrogenation of the Mg(NH₂)₂–2 LiH–0.1 Ca(BH₄)₂ composite are decreased by about 16.5 % and 28.1 %, respectively, and thus are responsible for the lower operating temperature and the faster dehydrogenation/hydrogenation kinetics. The fact that the hydrogen storage performances of the Ca(BH₄)₂‐doped sample are superior to the individually CaH₂‐ or LiBH₄‐doped samples suggests that the in situ formed CaH₂ and LiBH₄ provide a synergetic effect on improving the hydrogen storage properties of the Mg(NH₂)₂–2 LiH system.     

Synthesis of Ammonia Borane Nanoparticles and the Diammoniate of Diborane by Direct Combination of Diborane and Ammonia

Pure nanoparticle ammonia borane (NH₃BH₃, AB) was first prepared through a solvent‐free, ambient‐temperature gas‐phase combination of B₂H₆ with NH₃. The prepared AB nanoparticle exhibits improved dehydrogenation behavior giving 13.6 wt. % H₂ at the temperature range of 80–175 °C without severe foaming. Ammonia diborane (NH₃BH₂(μ‐H)BH₃, AaDB) is proposed as the intermediate in the reaction of B₂H₆ with NH₃ based on theoretical studies. This method can also be used to prepare pure diammoniate of diborane ([H₂B(NH₃)₂][BH₄], DADB) by adjusting the ratio and concentration of B₂H₆ to NH₃.     

Amminelithium Amidoborane Li(NH3)NH2BH3: A New Coordination Compound with Favorable Dehydrogenation Characteristics

The monoammoniate of lithium amidoborane, Li(NH₃)NH₂BH₃, was synthesized by treatment of LiNH₂BH₃ with ammonia at room temperature. This compound exists in the amorphous state at room temperature, but at ?20 °C crystallizes in the orthorhombic space group Pbca with lattice parameters of a=9.711(4), b=8.7027(5), c=7.1999(1) Å, and V=608.51 ų. The thermal decomposition behavior of this compound under argon and under ammonia was investigated. Through a series of experiments we have demonstrated that Li(NH₃)NH₂BH₃ is able to absorb/desorb ammonia reversibly at room temperature. In the temperature range of 40–70 °C, this compound showed favorable dehydrogenation characteristics. Specifically, under ammonia this material was able to release 3.0 equiv hydrogen (11.18 wt %) rapidly at 60 °C, which represents a significant advantage over LiNH₂BH₃. It has been found that the formation of the coordination bond between ammonia and Li⁺ in LiNH₂BH₃ plays a crucial role in promoting the combination of hydridic B? H bonds and protic N? H bonds, leading to dehydrogenation at low temperature.     

Effects of Stoichiometry on the H2‐Storage Properties of Mg(NH2)2–LiH–LiBH4 Tri‐Component Systems

The hydrogen desorption pathways and storage properties of 2 Mg(NH₂)₂–3 LiH–x LiBH₄ samples (x =0, 1, 2, and 4) were investigated systematically by a combination of pressure composition isotherm (PCI), differential scanning calorimetric (DSC), and volumetric release methods. Experimental results showed that the desorption peak temperatures of 2 Mg(NH₂)₂–3 LiH–x LiBH₄ samples were approximately 10–15 °C lower than that of 2 Mg(NH₂)₂–3 LiH. The 2 Mg(NH₂)₂–3 LiH–4 LiBH₄ composite in particular began to release hydrogen at 90 °C, thereby exhibiting superior dehydrogenation performance. All of the LiBH₄‐doped samples could be fully dehydrogenated and re‐hydrogenated at a temperature of 143 °C. The high hydrogen pressure region (above 50 bar) of PCI curves for the LiBH₄‐doped samples rose as the amount of LiBH₄ increased. LiBH₄ changed the desorption pathway of the 2 Mg(NH₂)₂–3 LiH sample under a hydrogen pressure of 50 bar, thereby resulting in the formation of MgNH and molten [LiNH₂–2 LiBH₄]. That is different from the dehydrogenation pathway of 2 Mg(NH₂)₂–3 LiH sample without LiBH₄, which formed Li₂Mg₂N₃H₃ and LiNH₂, as reported previously. In addition, the results of DSC analyses showed that the doped samples exhibited two independent endothermic events, which might be related to two different desorption pathways.     

Quantum mechanics investigation on initial decomposition of ammonia borane in glyme

The chemical kinetics of ammonia borane (AB) in glyme solution is studied using quantum mechanics (QM) based calculations along with experimental results available in the literature. The primary objective of this study is to propose a detailed reaction mechanism that explains the formation of species observed during AB decomposition for temperatures ranging from 323 to 368 K. The quantum mechanics investigation uses transition state theory to identify the relevant reaction pathways. Intrinsic reaction coordinate calculations use the identified transition‐state structure to link the reactants to the products. These calculations were performed using the Gaussian 09 program package, including the solvation model based on density (SMD) with acetonitrile as the solvent. Thermodynamic properties of species at equilibrium or at transition states were computed using the G4(MP2) compound method. Sensitivity analysis was performed using a species conservation model to identify reactions and species that play a critical role. This study confirms the previous experimental observation regarding the initiation of decomposition of AB in glyme. It also elucidates the role of DADB, ammonium borohydride salt ([BH₄]⁻[NH₄]⁺) and BH₂NH₂ in hydrogen release and intermediates formed during initial phase of AB decomposition. This work shows how QM calculations along with experimental results can contribute to our understanding of the complex chemical kinetics involved during AB dehydrogenation.     

Synthesis and Thermal Decomposition Behaviors of Magnesium Borohydride Ammoniates with Controllable Composition as Hydrogen Storage Materials

An ammonia‐redistribution strategy for synthesizing metal borohydride ammoniates with controllable coordination number of NH₃ was proposed, and a series of magnesium borohydride ammoniates were easily synthesized by a mechanochemical reaction between Mg(BH₄)₂ and its hexaammoniate. A strong dependence of the dehydrogenation temperature and purity of the released hydrogen upon heating on the coordination number of NH₃ was elaborated for Mg(BH₄)₂?x NH₃ owing to the change in the molar ratio of H^δ+ and H^δ?, the charge distribution on H^δ+ and H^δ?, and the strength of the coordinate bond N:→Mg²⁺. The monoammoniate of magnesium borohydride (Mg(BH₄)₂?NH₃) was obtained for the first time. It can release 6.5 % pure hydrogen within 50 minutes at 180 °C.     

Power‐Law Kinetic Models for Synthesis of Ammonia Borane

In the past few years, there have been increasing numbers of studies for the production and dehydrogenation of ammonia borane (NH₃BH₃, AB), which has become a significant hydrogen storage material. However, kinetic model studies based on the synthesis of AB in the literature have not been encountered, though there are many kinetic modeling studies on dehydrogenation of AB (Akbayrak et al., Appl Catal B 2016, 198, 162–170; Choi et al., Phys Chem Chem Phys 2014, 16(17), 7959–7968; Esteruelas et al., Inorg Chem 2016, 55(14), 7176–7181; Park et al., Int J Hydrogen Energy 2015, 40(46), 16316–16322; Rakap, Appl Catal B 2015, 163, 129–134; Tonbul et al., Int J Hydrogen Energy 2016, 41(26), 11154–11162; Zhang et al., Int J Hydrogen Energy 2016, 41(39), 17208–17215). The paper describes the development of a kinetic model for synthesis of ammonia borane by using borohydride (NaBH₄) and ammonium salt (NH₄)₂SO₄. The synthesis of AB experiments was carried out at different temperature ranges between 25 and 50°C, different inlet molar ratios (NaBH₄/(NH₄)₂SO₄ = 1–4), and different molarities with respect to NaBH₄ (0.11–0.67 M NaBH₄). After the parametric experiments were conducted, empirical power law was evaluated for the synthesis reaction. The power‐law model represented the trends of the kinetics of the synthesis reaction and was reproduced as .     

Formation and Unimolecular Dehydrogenation of Gaseous Alkaline‐earth Metal Amidoboranes M(NH2BH3)2 (M = Be – Ba): Comparative Computational Study

Formation of alkaline‐earth metal amidoboranes M(NH₂BH₃)₂ (M = Be, Mg, Ca, Sr, Ba) and unimolecular dehydrogenation reactions were computationally studied at the B3LYP/def2‐TZVPPD level of theory. Formation of M(NH₂BH₃)₂ from ammonia borane and MH₂ is exergonic, but subsequent unimolecular dehydrogenation reactions are endergonic at room temperature. In contrast to alkali metal amidoboranes, for M(NH₂BH₃)₂ the nature of M significantly affects their reactivity. Activation energies for the dehydrogenation of first and second hydrogen molecules decrease from Be to Ba. In case of Be compounds, intramolecular M ··· H–B contacts play an important role, whereas for heavier analogs such contacts are much less pronounced.