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1.
针对室温离子液体[bmim][BF4]和水的混合物, 用分子动力学模拟研究了溶液的微观组成与浓度的关系. 模拟结果表明:该混合物中各组分间的径向分布函数随[bmim][BF4]摩尔分数的增加呈有规律的变化;在此基础上计算了溶液的局部组成以及组分间的缔合因子, 进一步考察了各组分间的相互作用情况;另外基于Kirkwood-Buff理论估算了混合物的偏摩尔体积、等温压缩因子以及活度系数对浓度的偏导数, 对于理解离子液体与水之间的交互作用具有一定的参考意义.  相似文献   

2.
利用非等温、等温热重分析(TG)法,研究了高纯氮气气氛下1-丁基-3-甲基咪唑四氟硼酸盐([bmim][BF4])离子液体的热稳定性、平衡蒸汽压和标准蒸发焓.非等温热重(TG)曲线表明[bmim][BF4]的初始分解温度(Tonset)和最大分解速率对应的温度(Tm)分别为697和734K.然而长期等温TGA研究表明,[bmim][BF4]的最高可使用温度约为513K.另外,利用基于TG的蒸发技术研究了[bmim][BF4]的平衡蒸汽压(pe)与温度的关系并计算了标准蒸发焓.在503-543K温度范围内,离子液体[bmim][BF4]的pe和温度的关系是:lgpe=(16±1)+(-6.85±0.25)×103/T.[bmim][BF4]的标准蒸发焓为(131±5)kJ·mol-1.  相似文献   

3.
结合常规离子液体和功能型离子液体在吸收CO2方面的优势,将两类咪唑类离子液体进行混合,对其吸收CO2的效果和再生性能进行了实验研究。结果表明,两类咪唑类离子液体混合后流动性明显改善,与CO2接触气液传质顺畅;常规离子液体[bmim][BF4]和[bmim][Tf2N]与胺功能型离子液体[NH2e-mim][BF4]混合物较单一的离子液体吸收CO2的量大,[bmim][CH3CO2]与[NH2e-mim][BF4]混合后较单一的[bmim][CH3CO2]吸收量有明显的减低;随着常规咪唑类离子液体阳离子碳链增长,混合离子液体吸收CO2的效果变强;与胺乙基功能型离子液体混合吸收CO2时,阴离子为[Tf2N]的常规咪唑类离子液体要比阴离子为[BF4]的吸收效果好;离子液体混合物吸收CO2后经再生循环利用10次,混合物质量基本不变,循环使用后吸收CO2性能为初始吸收性能的75%~85%。  相似文献   

4.
建立了反相键合相液相色谱分析离子液体咪唑类离子液体[bmim]PF6[、bmim]BF4、吡啶类离子液体[bupy]BF4的纯度及其中高沸点有机物的方法.以缓冲溶液控制流动相pH值,显著改善了峰形.保留时间定性,外标法定量.  相似文献   

5.
室温离子液体由于其极低的蒸汽压、比较好的热稳定性和化学稳定性、良好的分子结构与性能的可设计性等优点,作为一种新型的环境友好溶剂在很多领域有着广泛的应用.对于离子液体的微观结构和微观性能的研究是设计新型离子液体以及扩展离子液体应用的关键.本文通过荧光探针分子香豆素153(C153)的转动动力学和对微观环境敏感的荧光探针分子1, 3-二(1-芘基)丙烷(BPP)的稳态荧光光谱,探测和表征了烷基取代的离子液体1-丁基-3-甲基咪唑六氟磷酸盐([bmim][PF6])和与其具有相似结构的醚键官能化的离子液体1-甲氧基乙基-3-甲基咪唑六氟磷酸盐([moemim][PF6])的微观结构和微粘度. C153探针分子在离子液体[bmim][PF6]中的转动过程具有快、慢两个组分表明离子液体[bmim][PF6]内部存在松散和紧密的两种结构微区;而C153探针分子在离子液体[moemim][PF6]中的转动动力学只存在一种过程,说明醚键的引入使得[moemim][PF6]内部趋于一种类型的微环境.通过C153探针分子的转动时间研究发现,醚键官能化的离子液体[moemim][PF6]的微粘度小于烷基链取代的离子液体[bmim][PF6],同时通过BPP探针分子的二聚体激基复合物(excimer)与单体(monomer)荧光发射强度的比值(IE/IM)研究也证明这一结果.醚键的引入使得离子液体[moemim][PF6]相对于离子液体[bmim][PF6],侧链的极性更大、柔顺性更好,同时醚键有可能作为氢键的受体与阳离子形成氢键从而削弱离子液体中阴、阳离子间的相互作用,使得离子液体[moemim][PF6]的微观环境比离子液体[bmim][PF6]更为均一,同时具有更小的微粘度.  相似文献   

6.
辣根过氧化物酶在亲水性离子液体中的活性与稳定性研究   总被引:3,自引:2,他引:1  
基于辣根过氧化物酶对过氧化氢氧化愈创木酚这个显色反应的催化作用,研究了辣根过氧化物酶在七种亲水性离子液体[C2mim][BF4]、[C4mim][BF4]、[C6mim][BF4]、[C4mim]HSO4、[C4mim]Cl、[C4mim]NO3、[C4mim][CF3CO2]中的活性与稳定性变化.结果表明辣根过氧化物酶在不同离子液体中均有不同程度的失活,辣根过氧化物酶活性随离子液体极性增强而降低.辣根过氧化物酶在含[C4mim]Cl离子液体的介质中,随着温度升高,[C4mim]Cl对辣根过氧化物酶的失活过程起加速作用,离子液体浓度越高,酶的热稳定性越差.紫外-可见光谱研究表明,在含[Cnmim][BF4]、[C4mim]HSO4、[C4mim]Cl、[C4mim]NO3的介质中,辣根过氧化物酶血红素中心最大吸收峰没有发生变化,但吸收值增强,证明离子液体使酶的血红素基团暴露于介质中而增强了吸收;而在含[C4mim][CF3CO2]的介质中,辣根过氧化物酶血红素基团最大吸收峰区发生蓝移,证明有部分血红素基团被离子液体破坏而脱落.  相似文献   

7.
应用荧光光谱、紫外吸收光谱、傅立叶变换红外光谱和核磁共振波谱研究了烷基咪唑型离子液体[bmim][PF6]及其前体物质[bmim]Cl与牛血清白蛋白(BSA)分子间的相互作用.研究表明:在生理pH值条件下,[ bmim][ PF5]和[bmim] Cl均对BSA的内源性荧光产生猝灭,其猝灭程度[bmim][ PF6]>...  相似文献   

8.
本文通过修饰阴阳离子合成了一系列咪唑型离子液体,以β-烯胺酮的合成为反应探针,考察离子液体结构和活性之间的关系。结果表明:阴阳离子对离子液体的活性都有显著的影响。阴离子为BF4-时,阳离子活性顺序为[Hmim]+[bmim]+,[emim]+[bmmim]+,其中[Hmim]BF4作反应介质,反应时间为10min,产率可达96%。当阳离子为[Hmim]+时,阴离子BF4-,Tsa-,Br-和NO3-活性均较高,产率达到93%以上,但阴离子HSO4-显著降低离子液体的活性,反应30min,产物收率仅有60%;阳离子为[bmim]+时,[bmim]Br[bmim]PF6[bmim]BF4,产率达到85%以上;而阴离子为HSO4-和H2PO4-时,离子液体活性变差,收率低于70%。离子液体[Hmim]BF4重复使用5次,β-烯胺酮产率基本不变,反应10min后,仍达89%。  相似文献   

9.
分子模拟研究气体在室温离子液体中的溶解度   总被引:2,自引:0,他引:2  
在作者先前建立的分子力场基础上, 采用Widom粒子插入法预测了CO2、N2、O2、Ar及CH4等5种气体在多种咪唑类离子液体中的溶解度, 包括2种侧链长度的阳离子和3种阴离子. 首先考察了256个离子对组成的体系中溶质分子插入次数对计算结果的影响, 在此基础上计算了不同温度下气体在1-丁基-3-甲基咪唑的四氟化硼盐([bmim][BF4])和六氟化磷盐([bmim][PF6])中的溶解度. 计算结果正确反映了CO2气体溶解度的变化趋势, 在[bmim][BF4]中溶解度的模拟结果与实验值符合很好, 且明显优于Pádua等的模拟结果;在[bmim][PF6]中的溶解度较实验值偏高, 精度与文献模拟结果相当;并预测了较高温度下CO2气体在[bmim][BF4]和[bmim][PF6]中的溶解度. 计算结果也正确地反映了5种气体在[bmim][PF6]中溶解度实验值的相对大小. 另外考察了常温下几种气体在不同室温离子液体中的溶解度, 模拟结果表明气体在含有较长碳链和双-三氟甲基磺酰胺阴离子(Tf2N)的离子液体中溶解度较大.  相似文献   

10.
将二醋酸纤维素(CDA)-(1-丁基-3-甲基咪唑四氟硼酸盐离子液体)([bmim]BF4)-肌红蛋白(Mb)的复合物修饰在玻碳电极(GCE)表面,制备了一种新型Mb修饰电极(CDA-[bmim]BF4-Mb/GCE).光谱分析表明:固定在CDA- [bmim]BF4-Mb膜中的肌红蛋白保持了其天然构象和生物活性.离子...  相似文献   

11.
The Kirkwood-Buff integrals of acetone-water mixtures are determined using two experimental techniques: small-angle neutron scattering and vapor pressure measurements, in order to test the precision and reliability that can be achieved. The data are then compared with those previously reported by different authors, which tend to show considerable variation between them. The various possible sources of inaccuracies are pointed out, both from experimental origins and from the numerical treatment of the data. Comparison with recent simulation results allows to critically compare different models and provide some information about the microstructure of the aqueous mixture.  相似文献   

12.
Several combinations of existing classical water and acetone models are studied by molecular dynamic simulations in order to sort out which models can reproduce available experimental data: enthalpies, pressure, densities, diffusion coefficients, and Kirkwood-Buff integrals. It turns out that all these properties, but the last, are rather well reproduced by all models, and with little numerical effort. By contrast, trials to measure by simulations the Kirkwood-Buff integrals lead to very long simulation times, thus revealing unexpected divergent behavior between the different models, such as phase separation, for example, and ultimately leading to a failure of any models combinations to reproduce these properties according to the experimental tendencies. It is argued herein that these deficiencies provide, in fact, an insightful picture of the microscopic structure of the solution, particularly into the relation between the hydrogen-bond network and the concentration fluctuations, as well as the role played by the solute in their spatial organization.  相似文献   

13.
The Kirkwood-Buff theory is applied to caffeine aqueous solution. The integrals of radial distribution functions are calculated from the osmotic coefficient, density and sound velocity data at 25°C. The results are discussed in terms of density fluctuations of two components and the correlation between them. It is found that the concentration dependence of Kirkwood-Buff integrals reflects the association tendency of caffeine and its strong influence on the properties of the solvent.  相似文献   

14.
The Kirkwood-Buff integrals of some binary aqueous alcohol mixtures are computed from the available vapor pressure measurements and compared with previous results as well as small angle neutron scattering experiments. The emphasis of the present report is on accuracy of the results that can be achieved by these two different types of measurements. This seems to be needed, mainly in view of the discrepancies between the various published results, as shown herein. It is argued that agreement in peak positions is more important than that in magnitude. In general, very good agreement is obtained by both methods, and sources of disagreements are discussed. The issue of the computer simulations of aqueous systems and the problematics related to correlations, microheterogeneity, and consequently the Kirkwood-Buff integrals are equally discussed herein.  相似文献   

15.
A formally exact Kirkwood-Buff virial formula for the surface tension of a supersaturated interface is derived. A modified Gibbs ensemble method is given that allows the creation of interacting supersaturated phases of equal chemical potential, and which enables the Kirkwood-Buff formula to be applied. The methods are tested by Monte Carlo simulation of a supersaturated Lennard-Jones fluid with a planar liquid-vapor interface. The Kirkwood-Buff results for the supersaturated surface tension are found to be in reasonable agreement with new results obtained here using the recently developed, formally exact, ghost interface method, [M. P. Moody and P. Attard, J. Chem. Phys., 2002, 117, 6705]. The surface tension is obtained as a function of supersaturation at four temperatures, and it is found to decrease with increasing supersaturation, and to vanish at the vapor spinodal. The relevance of the present results to the nucleation of droplets in a supersaturated vapor is discussed.  相似文献   

16.
We present a new tert-butanol force field parametrized to reproduce the mixture thermodynamics of tert-butanol/water over a wide range of solution compositions at room temperature and atmospheric pressure. The experimental Kirkwood-Buff integrals, which quantify preferential solvation of solution components by the same species or by the other components, were used as target values to be reproduced. Water was modeled using the simple point charge model. In the range of alcohol mole fractions between 0.02 and 0.98, our optimized model satisfactorily reproduces alcohol-alcohol, water-water, and alcohol-water aggregation behavior. As a consequence, the solution activity derivatives are reproduced as well. A comparison has been made with solution activities obtained by free energy calculations (i.e., thermodynamic integration). It clearly shows that the Kirkwood-Buff based approach performs superior in predicting solution activities of liquid mixtures. The new tert-butanol model has been used to examine the solution structure and hydrophobic interactions in aqueous tert-butanol at the various mixture compositions. A comparison is made with structural data obtained by neutron diffraction.  相似文献   

17.
Explicit expressions are developed for the chemical potential derivatives, partial molar volumes, and isothermal compressibility of solution mixtures involving four components at finite concentrations using the Kirkwood-Buff theory of solutions. In addition, a general recursion relationship is provided which can be used to generate the chemical potential derivatives for higher component solutions.  相似文献   

18.
19.
With the help of the Kirkwood-Buff theory of liquid mixtures it is demonstrated that there is a close relationship between, on the one hand, x-ray and neutron scattering intensities from liquid mixtures and, on the other hand, certain thermodynamic properties of the systems considered. This relationship can be utilized without having to specify the intermolecular interaction potential and without having to perform computer simulation calculations. In the present paper the Kirkwood-Buff theory is applied to liquid water and to the binary systems H2O/MeOH, H2O/EtOH, and cyclohexane/2,3-dimethyl-butane. On the basis of these examples it is explained that, from the thermodynamic quantities used, the detailed shape of the various molecular radial distribution functions cannot be established. However, in principle this information could well be obtained from the x-ray and neutron scattering intensities of the liquids that are being studied, provided an acceptable procedure could be found to isolate the different radial distribution functions. In this respect the information extracted from thermodynamic data would be essential since, in the first place, it provides a valuable way of normalization of the scattered intensity, and, in the second place, for multicomponent liquids it puts forward specific conditions to be satisfied by the various radial distribution functions.  相似文献   

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