稀散金属室温离子液体BMIInCl4的性质研究

在干燥高纯氩气氛的手套箱内,直接将摩尔比为1∶1的高纯无水InCl₃与氯化1-甲基-3-丁基咪唑(BM IC l)混合,得到无色透明的离子液体BM IInCl₄.在278.15-343.15 K温度范围内测定了该离子液体的密度和表面张力.利用G lasser经验方程和空隙模型讨论了BM IInCl₄的性质,并与离子液体BMIAlCl₄作了比较,证明了空隙模型具有一定的合理性.     

铝基离子液体BMIAlCl4的热力学性质

在高纯氩气氛下, 直接将摩尔比为1:1的高纯无水AlCl₃和BMIC(氯化1-甲基-3-丁基咪唑)搅拌混合, 得到一种无色透明的离子液体BMIAlCl₄. 在278.2～343.2 K范围内, 用最大气泡法测定了BMIAlCl₄的表面张力, 用Westphal天平法测定了该离子液体的密度；利用Glasser经验方程讨论了该离子液体的热力学性质, 并与其它离子液体作了比较. 根据空隙模型计算了BMIAlCl₄离子液体的恒压热膨胀系数, 与本文实验值基本一致, 说明空隙模型具有一定的合理性.     

利用标准加入法研究离子液体EMIBF4的密度和表面张力

在278.15～338.15 K温度范围内, 分别用Anton Paar密度计和最大气泡法测定了含有不同微量水的离子液体EMIBF₄ (1-ethyl-3-methylimidazolium tetrafluoroborate)的密度和表面张力, 讨论了微量水对这些性质的影响, 进而用标准加入法确定了无水离子液体EMIBF₄的密度和表面张力. 借助Glasser理论和空隙模型讨论了EMIBF₄的热力学性质. 用空隙模型计算的离子液体热膨胀系数与实验测定值较好一致, 说明空隙模型具有合理性.     

锌基离子液体BMIZn2Cl5的性质研究

合成了对水和空气均稳定的锌基离子液体五氯化二锌-1-甲基-3-丁基咪唑(BMIZn2Cl5). 在313.15～343.15 K温度范围内, 测定了离子液体BMIZn2Cl5的密度和表面张力. 拟合并估算了BMIZn2Cl5的恒压热胀系数和表面熵, 并根据Glasser理论和离子液体的空隙模型, 讨论了BMIZn2Cl5的热力学性质, 估算出其晶格能和标准熵 , 计算了离子液体的恒压热胀系数α, 与实验值基本一致, 说明了空隙模型的合理性. 并利用Kabo和Rebelo的方法估算了锌基离子液体BMIZn2Cl5的正常沸点, 蒸气压, 汽化焓( )等性质参数.     

锌基离子液体BMIZn2Cl5的性质研究

合成了对水和空气均稳定的锌基离子液体五氯化二锌-1-甲基-3-丁基咪唑(BMIZn2Cl5). 在313.15～343.15 K温度范围内, 测定了离子液体BMIZn2Cl5的密度和表面张力. 拟合并估算了BMIZn2Cl5的恒压热胀系数和表面熵, 并根据Glasser理论和离子液体的空隙模型, 讨论了BMIZn2Cl5的热力学性质, 估算出其晶格能和标准熵 , 计算了离子液体的恒压热胀系数α, 与实验值基本一致, 说明了空隙模型的合理性. 并利用Kabo和Rebelo的方法估算了锌基离子液体BMIZn2Cl5的正常沸点, 蒸气压, 汽化焓( )等性质参数.     

离子液体BMIBF4性质的研究

用最大气泡法和韦氏天平法, 在278.15～343.15 K范围内测定了离子液体BMIBF₄的表面张力和密度; 讨论了这个离子液体的体积性质和表面性质; 根据离子个头大又极不对称的特点, 提出了离子液体的空隙模型. 根据空隙模型计算的离子液体恒压热膨胀系数与实验值相比, 偏差在10%左右.     

离子液体四氟硼酸-1-戊基-3-甲基咪唑的物理化学性质的估算

根据标准加入法原理配制一系列含有已知微量水的离子液体四氟硼酸-1-戊基-3-甲基咪唑([C5mim][BF4])样品,在278.15～338.15 K温度范围内,样品的密度与其含水量呈很好线性关系. 利用外推方法确定了含水量为零时[C5mim][BF4]的密度ρ,得到了密度随温度变化的经验方程:ln ρ=0.120 11-5.79×10-4(T-298.15)和离子液体的热膨胀系数α=5.79×10-4K-1. 根据Glasser理论估算了[C5mim][BF4]的标准熵、表面能和晶格能,晶格能较小使离子液体在室温下能以液态形式存在. 利用空隙模型计算得到了[C5mim][BF4] 热膨胀系数α(计算),与实验测定值在数量级上一致,说明空隙模型有一定的合理性.     

咪唑基离子液体的物理化学性质估算及预测(英文)

根据经验和半经验方程及空隙模型理论,可以估算及预测离子液体在298.15K的物理化学性质.本文讨论了离子液体的分子体积,密度,标准熵,晶格能,表面张力,等张比容,摩尔蒸发焓,空隙体积,空隙率和热膨胀系数.通过实验测得的三种离子液体1-乙基-3-甲基咪唑硫酸乙酯([C2mim][EtSO4)]),1-丁基-3-甲基咪唑硫酸辛酯([C4mim][OcSO4])和1-乙基-3-甲基咪唑双三氟甲磺酰亚胺盐([C2mim][NTf2])的密度和表面张力估算了它们的其它物理化学性质.由这三种离子液体的分子体积及等张比容预测了同系列中其它离子液体[Cnmim][EtSO4],[Cnmim][OcSO4]和[Cnmim][NTf2](n=1-6)的分子体积及等张比容,由此计算出它们的密度及表面张力.进而预测了它们的物理化学性质.将预测的离子液体[C4mim][NTf2]和[C2mim][OcSO4]的密度值与文献报导的实验值进行比较,其偏差在实验误差范围内.最后,将由Kabo经验方程计算的七个离子液体[C2mim][EtSO4]、[C4mim][OcSO4]、[C2mim][NTf2]、[C4mim][NTf2]、丁基三甲基铵双三氟甲磺酰亚胺盐([N4111][NTf2])、甲基三辛基铵双三氟甲磺酰亚胺盐([N8881][NTf2])和1-辛基-3-甲基吡啶四氟硼酸盐([m3opy][BF4])的摩尔蒸发焓与由Verevkin简单规则预测的摩尔蒸发焓进行比较,发现两者符合很好.因此,在缺乏密度和表面张力实验数据的情况下,可以用Verevkin简单规则来预测离子液体的摩尔蒸发焓.     

离子液体BMIBF4性质的研究

用最大气泡法和韦氏天平法,在278．15～343．15K范围内测定了离子液体BMIBF4的表面张力和密度;讨论了这个离子液体的体积性质和表面性质;根据离子个头大又极不对称的特点,提出了离子液体的空隙模型．根据空隙模型计算的离子液体恒压热膨胀系数与实验值相比,偏差在10％左右。     

吡咯烷酮酸性离子液体的合成及其对酯化反应的催化活性

合成并表征了 2-吡咯烷酮硫酸氢盐([Hnhp]HSO4)、 1-甲基-2-吡咯烷酮硫酸氢盐([Hnmp]HSO4)、 1-甲基咪唑硫酸氢盐([Hmim]HSO4)、 1-(3-磺酸基)-丙基-3-甲基咪唑硫酸氢盐([C3SO3Hmim]HSO4)和1-(3-磺酸基)-丙基-2-吡咯烷酮硫酸氢盐([C3SO3Hnhp]HSO4)等以HSO-4为阴离子的质子酸离子液体,并以乙酸和正丁醇的酯化反应考察了这些离子液体的催化活性.结果表明,当n(n-BuOH):n(MeCO2H):n([C3SO3Hnhp]HSO4)=1.2:1:0.005,反应温度为120 ℃和反应时间为 1 h 时,酯收率可达99%以上;反应结束后离子液体与酯产物可分成两相,而且该离子液体重复使用8次,催化活性没有明显下降.探讨了阳离子结构及Brnsted酸性对催化活性的影响,考察了离子液体与酯化反应相关组分的互溶性.结果表明,离子液体的分相性能对催化效果有较大的影响,离子液体的催化活性与其酸性、溶解性密切相关.     

Studies on the properties of ionic liquid BMIInCl4

An ionic liquid (IL) was prepared by directly mixing InCl₃ and 1-methyl-3-butylimidazolium chloride(BMIC) with molar ratio 1:1 under dry argon atmosphere. The densities, and surface tension of pure IL were determined at temperature range of (278.15 to 343.15±0.1K). The properties for ionic liquid based on group III were discussed using Glasser’s theory. The standard entropy, the surface energy and the crystal energy of ionic liquid were calculated, respectively. The crystal energy of ionic liquid is much lower than ionic solid and this is the underlying reason for forming ionic liquid at room temperature. In addition, a new theoretical model of IL, that is interstice model, was applied to calculate the thermal expansion coefficient of BMIInCl₄. The order of magnitude for the thermal expansion coefficient, a, calculated by the theoretical model is in good agreement with experimental value. The result shows that there is much reasonableness for the interstice model of ionic liquid. __________ Translated from Chemical Journal of Chinese University, 2005, 26(10)(in Chinese)     

室温离子液体BMIGaCl4热力学性质研究

An ionic liquid （IL） BMIGaCh was prepared by directly mixing GaCl3 and 1-methyl-3-butylimidazolium chloride with molar ratio of 1/1 under argon atmosphere. The densities and surface tensions of this pure ionic liquid were determined in the temperature range of 268.15 to （338.15±0.1） K. A new theoretical model of ionic liquids, an interstice model, was applied to calculate the thermal expansion coefficient of IL BMIGaCh, a, and the magnitude order of its value calculated by the theory was the same as experimental one. Both Raman scattering and ab initio calculations indicate that GaCl4^- is the only species containing Ga in the ionic liquid BMIGaCl4.     

Estimation of physicochemical properties of ionic liquid C6MIGaCl4 using surface tension and density

An ionic liquid (IL) C6MIGaCl4 (1-methyl-3-hexylimidazolium chlorogallate) was prepared by directly mixing GaCl3 and 1-methyl-3-hexylimidazolium chloride with molar ratio of 1/1 under dry argon. The density and surface tension of the IL were determined in the temperature range of 283.15-338.15 K. The ionic volume and surface entropy of the IL were estimated by extrapolation, respectively. In terms of Glasser's theory, the standard molar entropy and lattice energy of the IL were estimated, respectively. By use of Kabo's method, the molar enthalpy of vaporization of the IL, Delta lgHm0 (298 K), at 298 K was estimated. According to the interstice model, the thermal expansion coefficient of IL C6MIGaCl4, alpha, was calculated and in comparison with experimental value; their magnitude order is in good agreement.     

Study on the properties of amino acid ionic liquid EMIGly

In terms of standard addition method, the density and surface tension of an amino acid ionic liquid EMIGly(1-ethyl-3-methylimidazolium aminoacetate) were measured under dry argon atmosphere in the temperature range of 288.15-343.15 K. The properties of volume and surface for pure EMIGly were discussed in terms of the interstice model and Glasser's theory. The thermal expansion coefficient alpha = 5.03 x 10(-4) K(-1) calculated using interstice model is in good agreement with alpha (experimental) = 5.20 x 10(-4) K(-1).     

Study on thermodynamic properties of a new air and water stable ionic liquid based on metal rhenium

A new air and water stable ionic liquid (IL) based on rhenium, N-butyl-pyridine perrhenate ([C₄Py][ReO₄]), was synthesized. The density and surface tension of the IL were determined over the temperature range of (293.15–343.15) K. In terms of the Glasser theory of IL and parachor, a series of physico-chemical properties: molecular volume, standard entropy, surface tension, and molar enthalpy of vaporization were predicted, respectively. According to the interstice model, the thermal expansion coefficient of the IL was calculated and in comparison with experimental value, it is in good agreement by 3.92%.