甘氨酸离子液体[C3mim][Gly]和[C4mim][Gly]水溶液的表面张力

本文用中和法合成了基于烷基咪唑的甘氨酸离子液体[C3mim][Gly]（1-丙基-3-甲基咪唑甘氨酸离子液体）和[c4miml[Gly]（1-丁基-3．甲基咪唑甘氨酸离子液体）,在298．15K下,0．0400-0．5000molkg^-1浓度范围内测定了不同浓度[C4mim][Oly]和[c3mim][Gly]离子液体水溶液的密度和表面张力,得到了溶液等张比容的实验值,提出了预测不同浓度溶液等张比容的经验方程,利用这个经验方程和李以圭等人提出的溶液表面张力模型,分别估算了这两种离子液体水溶液的表面张力,其估算值和实验值在误差范围内很好地吻合．     

离子液体[C2mim][GaCl4]的溶解热研究

在干燥氩气氛下, 用等摩尔的高纯无水GaCl3和[C2mim][Cl](氯化1-甲基-3-乙基咪唑)直接搅拌混合, 制备了淡黄色透明的的离子液体[C2mim][GaCl4] (1-ethyl-3-methylimidazolium chlorogallate) . 在298.15 K下, 利用具有恒温环境的溶解反应热量计, 测定了这种离子液体的不同浓度摩尔溶解焓 . 针对[C2mim][GaCl4]溶解于水后即分解的特点, 在Pitzer电解质溶液理论基础上, 提出了确定这种离子液体标准摩尔溶解焓的新方法, 得到了[C2mim][GaCl4]在水中的标准摩尔溶解焓, ＝－132 kJ•mol－1, 以及Pitzer焓参数组合: ＝－0.1373076和 ＝0.3484209. 借助热力学循环和Glasser离子液体晶格能理论, 用Ga3＋, Cl－和[C2mim]—的离子水化焓数据以及本文得到的[C2mim][GaCl4]标准摩尔溶解焓, 估算了配离子4Cl－(g)解离成Ga3＋(g)和4Cl－(g)的解离焓ΔHdis([GaCl4]-)≈5855 kJ•mol－1. 这个结果揭示了离子液体[C2mim][GaCl4]的标准摩尔溶解焓绝对值并不很大的原因, 即是很大的离子水化焓被很大的[GaCl4]－(g)的解离焓相互抵消了.     

过渡金属离子液体[C2mim][FeCl4]的溶解热

在干燥氩气氛下, 用等摩尔的高纯无水FeCl3和氯化1-甲基-3-乙基咪唑([C2mim][Cl])直接搅拌混合, 制备棕色透明的含过渡金属铁的离子液体[C2mim][FeCl4]. 在298.15 K下, 利用具有恒温环境的溶解反应热量计测定了这种离子液体的摩尔溶解焓(ΔsHm). 针对[C2mim][FeCl4]溶解于水后即分解的特点, 在Pitzer电解质溶液理论基础上, 提出了确定这种离子液体标准摩尔溶解焓的新方法, 得到了[C2mim][FeCl4]的标准摩尔溶解焓(ΔsH 0—m=-76.6 kJ/mol), 以及Pitzer焓参数组合: β(0)LFe,Cl+β(0)L[C2mim], Cl+ΦLFe,[C2mim]=0.072209和β(1)LFe,Cl+β(1)L[C2mim], Cl=0.15527. 借助热力学循环和Glasser离子液体晶格能理论, 用Fe3+, Cl-和[C2mim]+的离子水化焓数据以及[C2mim][FeCl4]标准摩尔溶解焓, 估算得到了配离子[FeCl4]-(g)解离成Fe3+(g)和4Cl-(g)的解离焓为5659 kJ/mol. 这个结果揭示了离子液体[C2mim][FeCl4]的标准摩尔溶解焓绝对值并不很大的原因, 即很大的离子水化焓被很大的[FeCl4]-(g)的解离焓相互抵消.     

[C4mim][PF6]和[C4mim][NTf2]离子液体辐射诱导的相行为及荧光行为变化

离子液体因其低挥发性, 高热稳定性及优良的萃取性能被认为是萃取分离放射性核素的新一代绿色溶剂, 而研究离子液体本身的辐射效应是其实际应用的重要前提. 本文以60Co为辐射源, 系统研究了γ辐照对两种常见的憎水性咪唑离子液体1-丁基-3-甲基咪唑六氟磷酸盐([C4mim][PF6])和1-丁基-3-甲基咪唑三氟甲基磺酰胺酸盐([C4mim][NTf2])的相行为及荧光行为的影响. 在相行为方面, γ辐照使离子液体的结晶驰豫时间增加, 导致其低温结晶延迟. 在荧光行为方面, γ辐照后离子液体的荧光光谱保持原有的“红边效应(red edge effect)”, 但随吸收剂量增加, 光谱整体发生红移(最大移动幅度达150 nm). 并且这种“红边效应”在辐照后离子液体的乙腈稀释剂中仍然存在, 且随稀释倍数增加光谱整体发生蓝移. [C4mim][PF6]和[C4mim][NTf2]离子液体辐照后的这种相行为及荧光行为的变化可归因于辐照对其阴阳离子空间相关性(缔合行为)的影响.     

丙氨酸离子液体[C4mim][Ala]的热化学性质

在298.15 K下利用恒温环境溶解热量计测定了一系列含有已知微量水的1-丁基-3-甲基咪唑丙氨酸盐([C₄mim][Ala])离子液体(IL)不同浓度样品的摩尔溶解焓. 借助Debye-Hückel极限项, 用外推法确定了不同含水量的[C₄mim][Ala]样品的标准摩尔溶解焓[Δ_sH_m⁰(wc)]. 随着样品中水含量的增加, Δ_sH_m⁰(wc)的绝对值下降, 将Δ_sH_m⁰(wc)对含水量作图得到很好的直线, 其截距Δ_sH_m⁰(pure IL)=-60.74 kJ/mol, 可看作是不含水的[C₄mim][Ala]标准摩尔溶解焓的估算值. 利用精密氧弹热量计测定了[C₄mim][Ala]的燃烧热, 计算得到其标准摩尔生成焓Δ_fH_m⁰=(-675±11) kJ/mol.     

咪唑类离子液体[C10mim][NTf2]萃取铈(IV)

以咪唑类离子液体1-癸基-3-甲基咪唑三氟磺酰亚胺盐[C10mim][NTf2]为萃取剂,研究了其对铈(Ⅳ)的萃取行为,分别考察了萃取时间、料液浓度、硝酸浓度、离子液体咪唑环上烷基链长、无机盐浓度和温度对萃取过程的影响。 热力学计算表明,萃取过程是自发的放热过程。 推测可能的萃取机理是阴离子交换机理。 对萃取液进行了反萃考察,在硫酸浓度为1.0 mol/L时,反萃率为85.1%。     

TODGA/[C_2mim][NTf_2]萃取Th~(4+)

研究了N,N,N′,N′-四辛基-3-氧戊二酰胺(TODGA)溶于疏水性离子液体咪唑类离子液体1-乙基-3-甲基咪唑双三氟甲磺酰亚胺盐([C2mim][NTf2])中对硝酸水溶液体系中四价钍离子(Th4+)的萃取行为。详细考察了接触时间、酸度、Th4+浓度、TODGA浓度、温度对TODGA/[C2mim][NTf2]体系萃取性能的影响。作为对比,我们还考察了TODGA在传统有机溶剂异辛烷中对Th4+的萃取。结果表明:TODGA/[C2mim][NTf2]体系对Th4+的萃取是吸热反应,且在50℃下,能在5 min内达到平衡。萃取体系随着酸度对Th4+的萃取性能先降后增大;Th4+浓度的增大,TODGA浓度的降低,对Th4+的萃取性能下降。TODGA在离子液体萃取体系中比在有机体系中有更好的Th4+萃取效果,特别是在低酸条件下。通过萃取机理研究,推测出在低酸下萃取反应是离子交换且TODGA与Th4+配比为2∶1,在高酸下萃取是中性配位。     

[C_4mim][PF_6]和[C_4mim][NTf_2]离子液体辐射诱导的相行为及荧光行为变化

离子液体因其低挥发性,高热稳定性及优良的萃取性能被认为是萃取分离放射性核素的新一代绿色溶剂,而研究离子液体本身的辐射效应是其实际应用的重要前提.本文以~(60)Co为辐射源,系统研究了γ辐照对两种常见的憎水性咪唑离子液体1-丁基-3-甲基咪唑六氟磷酸盐([C_4mim][PF_6])和1-丁基-3-甲基咪唑三氟甲基磺酰胺酸盐([C_4mim][NTf_2])的相行为及荧光行为的影响.在相行为方面,γ辐照使离子液体的结晶驰豫时间增加,导致其低温结晶延迟.在荧光行为方面,γ辐照后离子液体的荧光光谱保持原有的"红边效应(red edge effect)",但随吸收剂量增加,光谱整体发生红移(最大移动幅度达150 nm).并且这种"红边效应"在辐照后离子液体的乙腈稀释剂中仍然存在,且随稀释倍数增加光谱整体发生蓝移.[C_4mim][PF_6]和[C_4mim][NTf_2]离子液体辐照后的这种相行为及荧光行为的变化可归因于辐照对其阴阳离子空间相关性(缔合行为)的影响.     

[C3mim][NTf2]/DEC/[Li][NTf2]体系的基础性质

The hydrophobic ionic liquid (IL) 1-propyl-3-methylimidazolium bis[(trifluoromethyl)sulfonyl]imide ([C₃mim][NTf₂]) was synthesized according to traditional methods. By adding different amounts of diethyl carbonate (DEC) solvent and lithium bis[(trifluoromethyl)sulfonyl]imide ([Li][NTf₂]) salt to [C₃mim][NTf₂] IL, eight solution systems were prepared. First, the thermodynamic properties of the eight solution systems were characterized by differential scanning calorimetry (DSC). The semi-stable temperature of the system gradually disappeared with increasing lithium salt content, but the melting point temperature was not apparent in the experiment. These results indicate that DEC and lithium salts can dissolve in ILs within the tested temperature range. The basic properties of the eight systems, including thermodynamic and dynamic properties, were systematically studied at different temperatures. The variation in the self-diffusion coefficient of lithium ion ([Li]⁺) as a function of DEC concentration, density changes, viscosity, conductivity, and the viscosity/conductivity activation energy of the eight systems was calculated by the Vogel Fulcher Taman (VFT), Final Vogel Fulcher Taman (FVFT), and Arrhenius equations. The effect of temperature on the properties of the system was studied in detail. Within the temperature range measured herein, the deviation between the fitting equation and experimental value was small. Consequently, these equations were successfully used to calculate the properties of the system at various temperatures. All fitting parameters of the corresponding equations are provided herein. The viscosity for all systems decreased rapidly with increasing temperature, which increased the conductivity. Based on these experiments, the influence of DEC on the system microstructure was discussed in the context of the molecular dynamics simulation results. In particular, the interaction between [Li]⁺ and [NTf₂]^-/DEC was examined. In all solution systems, [NTf₂]^- coordinates to [Li]⁺ through only the O atom and not the N atom. Radial distribution function (RDF) analysis showed that the interaction between [Li]⁺ and [NTf₂]^- weakened with increasing DEC concentration. DEC molecules were observed in the first solvation layer of [Li]⁺ coordinating to [Li]⁺ through the carbonyl O atom. Although the interaction between [Li]⁺ and DEC was weakened, competition between [NTf₂]^- and DEC in the first solvation layer of [Li]⁺ was observed by the coordination number analysis of the O atom around [Li]⁺. Therefore, the introduction of DEC is beneficial for Li⁺ diffusion, which is consistent with the experimental results.     

γ辐射下CMPO/[C2mim][NTf2]的辐解及其对Eu3+萃取的影响

主要考察了辛基(苯基)-N, N-二异丁基胺甲酰基甲基氧化膦(CMPO)在1-乙基-3-甲基咪唑双三氟甲基磺酰胺酸盐([C₂mim][NTf₂])中的γ辐解行为,同时考察辐射对CMPO/[C₂mim][NTf₂]萃取能力的影响。通过超高效液相色谱-四极杆飞行时间质谱联用仪(UPLC/Q-TOF-MS)进行定量分析、辐解产物认定以及产物半定量分析。CMPO/正十二烷作为对比条件进行了相同研究。结果表明：CMPO在[C₂mim][NTf₂]中的辐解率低于其在正十二烷中,并且辐解路径不同。在正十二烷体系中,CMPO主要发生C―P、C―N键的断链,而在离子液体体系中CMPO主要发生异丁基脱除反应,并与[C₂mim]^+·、·CF₃等离子液体产生的自由基发生取代反应。综合辐解研究结果,我们提出CMPO/[C₂mim][NTf₂]的辐解路径,这加深了CMPO在离子液体中辐解机理的认识。最后,通过萃取实验发现,当硝酸浓度为0.01 mol·L^-1,辐照剂量为800 kGy时,CMPO/[C₂mim][NTf₂]对Eu³⁺的萃取率依旧达到99%以上。     

醋酸离子液体[C2mim][OAc]水溶液的摩尔表面Gibbs自由能

在288.15-318.15 K温度范围内测定了不同浓度离子液体1-乙基-3-甲基咪唑醋酸盐([C₂mim][OAc])水溶液的表面张力和密度;在改进李以圭等人的溶液表面张力模型基础上,提出摩尔表面Gibbs自由能新概念,建立了摩尔表面Gibbs自由能随溶液浓度变化的线性经验方程,利用这个经验方程估算了[C₂mim][OAc]水溶液的摩尔表面Gibbs自由能,并进一步预测了该溶液的表面张力,其预测值与相应的表面张力实验值高度相关并非常相似。由此可见,摩尔表面Gibbs自由能与等张比容极其类似,可能成为预测离子液体及其溶液性质的一种新的半经验方法。在指定溶液浓度下,根据溶液的摩尔表面Gibbs自由能随温度呈线性变化的规律,得到了新的Eötvös方程,与传统的Eötvös方程相比,新Eötvös方程的每一个参数都有明确的物理意义:斜率的负值是摩尔表面熵,截距是摩尔表面焓,在指定浓度的溶液中摩尔表面焓几乎不随温度变化。     

用核磁共振技术研究[C4mim][BF4]在重水和氘代氯仿中的聚集行为

运用核磁共振技术,研究了室温离子液体1-丁基-3-甲基咪唑四氟硼酸盐([C4mim[BF4])在重水和氘代氯仿中的聚集行为.实验结果表明,随着混合体系中离子液体摩尔分数的增加,在重水中,离子液体阳离子上各氢原子的化学位移向低场移动,且呈现了先急剧变化,后趋于平缓的变化趋势;在氘代氯仿中,离子液体阳离子上H2的化学位移向高场移动,H4和H5以及与氮原子直接相连的甲基和亚甲基上的氢原子的化学位移都向低场移动,且各氢原子的核磁共振信号发生了变化.根据质量作用定律及1H NMR化学位移随浓度的变化关系计算了[C4mim][BF4]在重水中的临界聚集浓度和聚集数,并在离子液体阴、阳离子缔合以及离子液体与溶剂相互作用的基础上对实验结果进行了讨论.     

Synthesis,Crystal and Molecular Structures of [Co(MH)2(Thio)2][BF4] · H2O and [Co(DH)2(NH3)2][BF4]

Crystal structures of [Co(MH)₂(Thio)₂][BF₄] · H₂O (I) and [Co(DH)₂(NH₃)₂][BF₄] (II), where MH^– is H₃C–C(NOH)–C(NO^–)–H and DH^– is H₃C–C(NOH)–C(NO^–)–CH₃, were determined by X-ray diffraction. The crystals are monoclinic, space group C2/c, unit cell parameters (for I and II, respectively): a = 22.018(2) Å, b = 7.943(1) Å, c = 11.681(1) Å, = 92.68(1)° and a = 21.436(2) Å, b = 6.400(2) Å, c = 12.389(2) Å, = 113.13(1)°. In both cases, the Co(III) coordination polyhedron is a centrosymmetrical trans-octahedron, N₄S₂ for I and N₆ for II. In the crystals of I and II, the complex cations and the outer-sphere [BF₄]^– anions (and the crystal water molecules in I) form elaborate hydrogen bonding system.     

用核磁共振技术研究[C4mim][BF4]在重水和氘代氯仿中的聚集行为

运用核磁共振技术, 研究了室温离子液体1-丁基-3-甲基咪唑四氟硼酸盐([C4mim][BF4])在重水和氘代氯仿中的聚集行为. 实验结果表明, 随着混合体系中离子液体摩尔分数的增加, 在重水中, 离子液体阳离子上各氢原子的化学位移向低场移动, 且呈现了先急剧变化, 后趋于平缓的变化趋势; 在氘代氯仿中, 离子液体阳离子上H2的化学位移向高场移动, H4和H5以及与氮原子直接相连的甲基和亚甲基上的氢原子的化学位移都向低场移动, 且各氢原子的核磁共振信号发生了变化. 根据质量作用定律及1H NMR化学位移随浓度的变化关系计算了[C4mim][BF4]在重水中的临界聚集浓度和聚集数, 并在离子液体阴、阳离子缔合以及离子液体与溶剂相互作用的基础上对实验结果进行了讨论.     

气态二聚体[C1~6mim]2[BF4]2纳米微观结构的理论研究

在B3LYP/6-311+G(d,p)的水平上采用密度泛函理论研究了[C_nmim]+(n=1~6)与[BF_4]~ˉ形成二聚体[C_nmim]_2[BF_4]_2(n=1~6)的微观纳米结构。通过理论计算二聚体的相互作用能量发现,阴阳离子之间存在较强的氢键作用,且随着咪唑鎓烷基链的增加相互作用能也随之增加,另外,烷基侧链的长度会影响氢键强度。当咪唑鎓烷基侧链中C的个数大于4时,烷基尾部能够发生聚合,从而形成类胶束纳米结构。通过对自然布居分析、自然键轨道以及弱相互作用的分析和计算,同样证明了二聚体中存在较强的氢键作用,烷基侧链中碳的个数影响了离子液体的微观结构。     

Synthesis and structure of tetra-p-tolylantimony complexes [(4-MeC6H4)4Sb] 2 + [Hg2I6]2−, [(4-MeC6H4)4Sb] 2 + [HgI4]2−, [(4-MeC6H4)4Sb] 3 + [Sb3I12]2−, and [(4-MeC6H4)4Sb]+[ReO4]−

Complexes [(4-MeC₆H₄)₄Sb] ₂ ⁺ [Hg₂I₆]^2? (I), [(4-MeC₆H₄)₄Sb] ₂ ⁺ [HgI₄]^2? (II), [(4-MeC₆H₄)₄Sb] ₃ ⁺ [Sb₃I₁₂]^2? (III), were synthesized by reactions of tetra-p-tolylantimony iodide with mercury iodide and antimony iodide, respectively. Tetra-p-tolylantimony perrhenate [(4-MeC₆H₄)₄Sb]⁺[ReO₄]^? (IV) was prepared from tetra-p-tolylantimony chloride and sodium perrhenate in acetone. Crystal structures of complexes I, II, and IV were determined by X-ray crystallography. Mercury and rhenium atoms have tetrahedral coordinations in these complexes. The Hg-I and Re-O distances in the structures of I, II, and IV vary within 2.7719(13)–2.7908(12)Å, 2.7028(3)–2.9163(3) Å, and 1.693(3)–1.744(3) Å, respectively. Antimony atoms in two crystallographically independent trinuclear centrosymmetric [Sb₃I₁₂]^2? anions of complex III have an octahedral environment. Each terminal SbI₃ fragment (Sb-I_t, 2.8265(9)–2.8333(10)Å) is bound to the central atom through tree bridging iodine atoms (Sb(2)-I_br, 3.2275(9)–3.3620(10)Å). The distances between the central Sb atom and bridging iodine atoms are much shorter (Sb(1)-I_br, 3.0153(6)–3.0316(6) Å; Sb(3)-I_br, 2.9926(6)–3.0074(6) Å).     

Synthesis and structure of antimony complexes [Ph3AmP] 2 + [Sb2I8 · 2DMSO]2−, [Ph3PrP] 2 + [Sb2I8 · C4H8O2]2−, and [(HOCH2CH2)3NH] 4 + [Sb4I16]4−

The reaction of equimolar amounts of triphenylamyl- and triphenylpropylphosphonium iodides and triethanolammonium iodide with antimony iodide in dimethyl sulfoxide, dioxane, or acetone gave complexes [Ph₃AmP] ₂ ⁺ [Sb₂I₈ · 2DMSO]^2?, [Ph₃PrP] ₂ ⁺ [Sb₂I₈ · C₄H₈O₂]^2?, and [(HOCH₂CH₂)₃NH] ₄ ⁺ [Sb₄I₁₆]^4?, the structure of which was established by X-ray diffraction analysis. The cations of all complexes have slightly distorted tetrahedral structure, and the antimony atoms in the anions are hexacoordinated. The crystals of the complexes have intra- and intermolecular contacts, which form the structure.     

1-甲基-3-乙基咪唑缬氨酸盐离子液体[C2mim][Val]的热化学

用中和法合成了氨基酸离子液体1-甲基-3-乙基咪唑缬氨酸盐([CB_2Bmim][Val]). 在298.15±0.01 K下, 利用恒温溶解反应热量计测定了不同含水量的[CB_2Bmim][Val]溶解成不同质量摩尔浓度溶液的溶解焓, ΔB_solBHB_mB (w), 借助标准加入法(SAM)和Archer方法得到了无水离子液体[CB_2Bmim][Val]的标准摩尔溶解焓, . 利用RB-II型精密转动弹热量计测定了该离子液体的燃烧热, 计算了其标准摩尔燃烧焓 和标准摩尔生成焓 |并结合该离子液体的标准摩尔溶解焓和乙基咪唑阳离子[CB_2Bmim]^＋在水溶液中的标准摩尔生成焓, 计算了[Val]P^－离子在水溶液中的标准摩尔生成焓. 利用RD496-III型热导式微量热量计测定了不同质量摩尔浓度[CB_2Bmim][Val]水溶液的稀释焓, 根据扩展的Debye-Hückel方程计算得到的相对表观摩尔焓P^φPL和根据Pitzer离子相互作用模型的计算值在实验误差范围内很好一致.     

Synthesis of open-framework iron phosphates, [C5N2H14]2[FeIII2F2(HPO4)4]·2H2O and [C5N2H14][FeIII4(H2O)4F2(PO4)4], with one- and three-dimensional structures

The hydrothermal syntheses and structures of two new open-framework iron phosphates, [C₅N₂H₁₄]₂[Fe^III₂F₂(HPO₄)₄]·2H₂O, I, and [C₅N₂H₁₄][Fe^III₄(H₂O)₄F₂(PO₄)₄], II, are presented. While the structure of I consist of FeO₄F₂ octahedra and HPO₄ terahedra linked to form one-dimensional structure, that of II consist of FeO₄(H₂O)₂, FeO₄(H₂O)F, FeO₄F₂ and PO₄ units connected to give rise to a three-dimensional structure. The structure of I resembles the naturally occurring mineral tancoite while II resembles the iron phosphate, ULM-12, [C₆N₂H₁₄][Fe₄(PO₄)₂F₂(H₂O)₃]. Magnetic susceptibility studies indicate anti-ferromagnetic behavior in both the compounds with T_N=200 and 175 K for I and II, respectively. Crystal data: I, monoclinic, space group=P2₁/n (no. 14). a=7.2261(6), b=16.5731(14), c=11.0847(10) Å, β=97.265(2)°, V=1316.8(2) Å³, Z=4, ρ_calc=1.952 g cm⁻¹, μ_(MoKα)=1.446 mm⁻¹, R₁=0.0448 and wR₂=0.1141 for 1882 data [I>2σ(I)]; for II, monoclinic, space group=P2₁/n (no. 14). a=9.9691(3), b=12.4013(3), c=17.3410(3) Å, β=103.762(1)°, V=2082.32(9) Å³, Z=4, ρ_calc=2.576 g cm⁻¹, μ_(MoKα)=3.162 mm⁻¹, R₁=0.0510 and wR₂=0.1064 for 2979 data [I>2σ(I)].