某些非极性和极性溶质在苯和甲醇及二者混合物中的偏摩尔体积V~0,298.15K

密度法测定了298.15K下乙醇、环己烷、三氯甲烷、甲苯、丙酮、四氯化碳、乙腈、二甲基甲酰胺、二甲基亚砜在甲醇或苯及两者混合物中的无限稀释偏摩尔体积.密度测定所用溶液中溶质的浓度范围是0.2一1.5m;甲醇和苯混合物是全组成比范围.溶质偏摩尔体积随甲醇-苯组成比的变化趋势反映了几种分子间相互作用结果即三种分子间物理型分子间相互作用;溶质与甲醇分子氢键缔合相互作用;溶质同甲醇或苯的弱络合作用。     

某些非极性和极性溶质在苯和甲醇及二者混合物中的偏摩尔体积V0, 298.15 K

密度法测定了298.15 K下乙醇、环己烷、三氯甲烷、甲苯、丙酮、四氯化碳、乙腈、二甲基甲酰胺、二甲基亚砜在甲醇或苯及两者混合物中的无限稀释偏摩尔体积. 密度测定所用溶液中溶质的浓度范围是0.2一1.5 m; 甲醇和苯混合物是全组成比范围. 溶质偏摩尔体积随甲醇-苯组成比的变化趋势反映了几种分子间相互作用结果即三种分子间物理型分子间相互作用; 溶质与甲醇分子氢键缔合相互作用; 溶质同甲醇或苯的弱络合作用。     

混合超临界流体的密度及分子间相互作用

在３０８．１５Ｋ、６－１２ＭＰａ范围内,测定了ＣＯ２及ＣＯ２－正戊烷、ＣＯ２－正庚烷二元混合流体的密度,并计算了溶质的偏摩尔体积．在此基础上,将偏摩尔体积与ＭｏｎｔｅＣａｒｌｏ分子模拟研究相结合,研究了ＣＯ２－正戊烷、ＣＯ２－正庚烷二元系中的分子间相互作用和溶液的结构随压力和密度的变化．     

甲酰胺、乙酰胺、尿素在两种极性非水溶剂中的体积性质

以尿素、甲酰胺和乙酰胺为溶质,二甲基甲酰胺和二甲基亚砜为溶剂;或以二甲基甲酰胺、二甲基亚砜为溶质,以甲酰胺为溶剂,通过测定溶液在２９８．１５Ｋ下的密度数据,求得了溶质的表观摩尔体积以及与溶质－溶质相互作用相关的体积第二维里系数．利用定标粒子理论讨论了溶质分子的几何体积、溶质－溶剂相互作用对溶质偏摩尔体积的影响,结果表明,溶质的溶剂化与溶质－溶质相互作用的体积效应呈相反的变化趋势     

NaCl、KCl在蔗糖水溶液中的粘度

报导了在298．15及308．15K下，NaCl、KCl在含有蔗糖5，10，15，20，25％（质量分数w）的水溶液中的密度及粘度数据．计算了在无限稀释条件下，NaCl和KCl在该体系中的粘度B系数及偏摩尔体积．结果发现：两种电解质的B系数随蔗糖含量的增加及温度的升高而增大且对蔗糖水溶液的结构起破坏作用．讨论了该三元体系内部溶质－溶质、溶质－溶剂间的相互作用，同时应用流动过渡状态理论计算了两种电解质在各组成下蔗糖水溶液中的流动活化参数     

D-甘露醇在正丙醇和异丙醇水溶液中的体积性质

使用石英振荡管密度计精确测定了298.15K温度下不同浓度的甘露醇-正丙醇-水和甘露醇-异丙醇-水三元溶液的密度.计算了甘露醇的表观摩尔体积VΦ和极限偏摩尔体积VΦ,得到了其由纯水溶剂转移至混合溶剂中的迁移偏摩尔体积ΔtrsVΦ.结果表明,正丙醇在溶液中对甘露醇体积性质的影响较异丙醇显著.从溶质-溶剂分子间相互作用及丙醇同分异构体中羟基位置的不同对体积性质的变化规律进行了讨论.     

甲酰胺,乙酰胺,尿素在两种极性非水溶液中的体积性质

以尿素、甲酰胺和乙酰胺为溶质，二甲基甲酰胺和二甲基亚砜为溶剂；或以二甲基甲酰胺、二甲基亚砜为溶质，以甲酰胺为溶剂，通过测定溶液在２９８．１５Ｋ下的密度数据，求得了溶质的表观磨尔体积以及与溶质－溶质相互作用相关的体积第二维里系数。利用定标粒子理论讨论了溶质分子的几何体积、溶质－溶剂相互作用对溶质偏摩尔体积的影响，结果表明，熔质的溶剂化与溶质－溶质相互作用的体积效应呈相反的变化趋势。     

氨基酸在水或氯化钾水溶液中体积性质的研究

在298.15K和常压下利用密度法测定了十几种α-氨基酸在水或氯化钾水溶液中的表观摩尔体积, 由此得到了各氨基酸的偏摩尔体积和其相应的转移偏摩尔体积,以及氨基酸中侧链对其偏摩尔体积的贡献值。从理论上计算了各氨基酸在上述溶液浓度的增加而增大; 氨基酸共溶质间的相互作用以1:1形式为主; 氨基酸的水化数随盐浓度的增加而减小。对所得结果进行了定性讨论。     

氨基酸在水或氯化钾水溶液中体积性质的研究

在298.15K和常压下利用密度法测定了十几种α-氨基酸在水或氯化钾水溶液中的表观摩尔体积,由此得到了各氨基酸的偏摩尔体积和其相应的转移偏摩尔体积,以及氨基酸中侧链对其偏摩尔体积的贡献值.从理论上计算了各氨基酸在上述溶液中的水化数和体积相互作用参数.结果表明,氨基酸的转移偏摩尔体积值随着盐溶液浓度的增加而增大;氨基酸与共溶质间的相互作用以1∶1形式为主;氨基酸的水化数随盐浓度的增加而减小.对所得结果进行了定性讨论.     

I>D-甘露醇在正丙醇和异丙醇水溶液中的体积性质

使用石英振荡管密度计精确测定了298.15 K温度下不同浓度的甘露醇-正丙醇-水和甘露醇-异丙醇-水三元溶液的密度. 计算了甘露醇的表观摩尔体积V_Φ和极限偏摩尔体积, 得到了其由纯水溶剂转移至混合溶剂中的迁移偏摩尔体积. 结果表明, 正丙醇在溶液中对甘露醇体积性质的影响较异丙醇显著. 从溶质-溶剂分子间相互作用及丙醇同分异构体中羟基位置的不同对体积性质的变化规律进行了讨论.     

Apparent molar volumes of lithium nitrate in 1-propanol + water in the temperature range from 288.15 to 318.15 K

Densities of 1-propanol+water+lithium nitrate mixtures have been measured with an oscillating-tube densimeter over a large range of concentrations of the salt and 1-propanol, at 288.15, 298.15, 308.15, and 318.15 K. From these densities, apparent molar volumes of lithium nitrate in 1-propanol+water mixtures have been calculated for each temperature, and apparent molar volumes at infinite dilution have been evaluated. An empirical correlation for partial molar volumes of lithium nitrate in 1-propanol+water mixtures with solvent composition and temperature has been derived.     

Effect of Molecular Size of Solutes on Their Partial Molar Volumes in Supercritical n-Pentane

Supercritical fluids (SCFs) have many unique properties1. However, nearly all of the features are related with the aggregation or clustering of the molecules in the fluids. Some researchers have reported that the partial molar volumes (PMVs) of the solutes in dilute supercritical (SC) solutions are large negative values1-4, which is different from common liquid solutions. Negative PMV of a solute in SC solution results from the fact that the local density of the solvent surrounding the so…     

Volumes,heat capacities,and compressibilities of the mixtures of acetonitrile and 2-methoxyethanol

Heat capacities and speed of sound of (acetonitrile + 2-methoxyethanol) mixtures at 298.15 K and the densities of the same mixtures at T = (308.15 and 318.15) K were determined over the whole composition range. The excess of molar volume and isobaric heat capacity of the mixture, the partial molar volumes and heat capacities of both components of the mixture as well as the adiabatic and isothermal coefficients of compressibility and their excess were calculated from the obtained experimental data. The internal pressure of the examined system was also calculated. The results of investigations were analyzed and discussed. The behavior of the analyzed functions is similar to that observed in the case of the mixtures of acetonitrile with some aprotic solvents examined earlier.     

Density of supercritical CO_2-tetrahydrofuran binary mixture and the partial molar volume of the cosolvent

The densities of supercritical CO2-tetrahydrofuran (cosolvent) binary mixture weremeasured at temperatures in range of 308.15 to 323.15 K and at pressure up to 16.5 MPa.The concentrations of tetrahydrofuran were from 0 to 0.57 mol/L.The partial molar volume of tetrahydrofuran was calculated based on the relationship between the density of the mixture and the concentration of the cosolvent.It is observed that the partial molar volume of the cosolvent is negative and the absolute value decreases with increasing pressure and the concentration of the cosolvent.     

Studies of Associated Solutions: Evaluation of Thermodynamic Parameters of Blends of 2-Methylaniline and Substituted Ethanols at Various Temperatures

Densities (ρ), speeds of sound (u), and viscosities (η) are reported for binary mixtures of 2-methylaniline with substituted ethanols (2-phenylethanol, 2-chloroethanol and 2-aminoethanol) over the entire composition range of mole fraction at T?=?(303.15–318.15) K and at atmospheric pressure, 0.1 MPa. The excess molar volume, excess isentropic compressibility and deviation in viscosity are calculated from the corresponding experimental densities, speeds of sound and viscosities. The excess properties are correlated using the Redlich–Kister polynomial smoothing equation. Excess partial molar volumes and excess partial molar isentropic compressibilities were calculated for all the binary systems throughout the composition range and also at infinite dilution. The variations in these properties with composition, for all the binary mixtures, suggest that loss of dipolar association, difference in size and shape of the component molecules, dipole–dipole interaction and hydrogen bonding between molecules of 2-methylaniline with 2-phenylethanol, 2-chloroethanol and 2-aminoethanol are involved.     

Density and Refractive Index for Binary Systems of the Ionic Liquid [Bmim][BF<Subscript>4</Subscript>] with Methanol, 1,3-Dichloropropane,and Dimethyl Carbonate

Refractive indices at 298.15 K and densities in the temperature interval 293.15 to 318.15 K were determined at atmospheric pressure over the whole composition range for the binary systems [Bmim][BF₄]+(methanol, or 1,3-dichloropropane, or dimethyl carbonate). Due to the high viscosity of the samples, which would produce a wrong density if a classical vibrating-tube densimeter were used, a densimeter was employed that automatically corrects the data for the viscosity effect. Because at room temperature some [Bmim][BF₄]+dimethyl carbonate mixtures showed partial immiscibility, liquid-liquid equilibrium was determined for this system. Excess molar volumes and deviations of refractive index from linear mixing behavior were calculated from the experimental data. An erratum to this article can be found at     

Volumetric properties of aqueous electrolytes at high temperature. II. B(OH)3 and B(OH)3−NaB(OH)4−NaOH mixtures up to 523 K

The densities of boric acid aqueous solutions and sodium hydroxide-sodium borate mixtures were measured as a function of concentration, between 375 and 523 K at pressures close to saturation. The partial molar volumes of boric acid were obtained and it was found that they are almost independent of the concentration. The partial molar volumes of the sodium hydroxide-sodium borate mixtures were fitted to the Pitzer equation for mixtures using the known parameters for NaOH. Thus, the partial molar volume at infinite dilution and the Pitzer parameters of sodium borate could be obtained by assuming ideal mixing.     

Volumetric Properties of Sodium Chlorobenzoate in N,N Dimethylformamide/water Mixtures at 298.15 K

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The bulk properties of ethylene glycol-dimethylsulfoxide mixtures over the temperature range 278–323 K at <Emphasis Type="Italic">p</Emphasis> = 0.1 MPa

The densities of ethylene glycol-dimethylsulfoxide binary mixtures were measured over the temperature range 278–323.15 K at atmospheric pressure using a vibrational densimeter. The excess molar volumes, apparent molar volumes, partial molar volumes of mixture components, volumetric thermal expansion coefficients, and partial molar volumetric thermal expansion coefficients were calculated. The excess molar volumes were described by the Redlich-Kister equation, and the partial molar volumes were calculated by two methods. The density-composition dependence contained a weak maximum, which disappeared as the temperature increased. The excess molar volumes were negative, and deviations from ideality increased as the temperature grew.